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© Emna Ghazali, 2017
Mechanical performance of adhesively bonded repairs in honeycomb composite sandwich structures
Thèse
Emna Ghazali
Doctorat en génie mécanique
Philosophiæ doctor (Ph. D.)
Québec, Canada
Mechanical Performance of Adhesively Bonded Repairs in Honeycomb Composite Sandwich Structures
Thèse
Emna Ghazali
Sous la direction de :
Marie-Laure Dano, directrice de recherche
Augustin Gakwaya, codirecteur de recherche
iii
Résumé
En service, les pièces aéronautiques en matériaux composites et structures sandwiches
subissent des dommages qui nécessitent des réparations. Les réparations par patch interne en
biseau, en escalier ou par combinaison des deux offrent une excellente restauration de la
résistance mécanique pour ces structures composites. Cependant, l’environnement de
réparation peut se révéler être un défi de taille quant à leur mise en œuvre, au choix des
paramètres géométriques (angle de biseau, nombre de plis extra), à leur comportement
mécanique sous différents chargements ainsi qu’à leur processus d’endommagement.
Cette thèse présente une étude expérimentale et numérique (éléments finis) du comportement
mécanique de réparations par patch interne effectuées sur des structures avec des peaux en
composites à renforts tissés fabriquées hors autoclave et âme en Nomex en nid d’abeille. Afin
de déterminer l’effet de différents paramètres géométriques sur la résistance de la réparation et
de comprendre son comportement mécanique et son processus d’endommagement, une série
de tests de caractérisation sous différents chargements (traction, compression, flexion) a été
effectuée sur des structures sandwiches faite avec deux matériaux composites tissés pour la
peau : soit du composite tissé taffetas (PW) ou satin de 8 (8HS)
Des simulations numériques ont été effectuées afin de prédire le comportement mécanique de
la réparation. Cette étude numérique a été effectuée en plusieurs étapes. Un premier modèle
iv
2D qui suppose que la colle ait un comportement linéaire élastique a été développé et permet
d’étudier la distribution des contraintes dans le joint de colle pour différentes configurations de
réparation rectangulaire. Ensuite, le modèle 2D est modifié pour tenir compte du comportement
élastoplastique de la colle et ceci permet de prédire le comportement mécanique d’une
réparation rectangulaire jusqu’à la rupture. Par la suite, un modèle 3D est développé pour
prédire le comportement de réparations circulaires sous des chargements de compression. Ce
modèle tient compte de l’endommagement progressif des peaux en composite. Les résultats de
ces simulations numériques sont comparés par la suite aux mesures expérimentales. Les
modèles par éléments finis, avec une loi de comportement élastoplastique pour le joint de colle,
permettent une estimation adéquate de la résistance ainsi que de l’endommagement des
structures sandwiches réparées. Une étude paramétrique a eu lieu afin d’étudier l’effet de
différents paramètres géométriques sur la résistance de la réparation.
La mise en œuvre et la détermination de la performance mécanique des réparations par patch
interne des structures sandwiches est une tâche complexe avec de multiples paramètres de
matériaux et de procédés. D’une manière générale, cette thèse contribue à une meilleure
compréhension du comportement mécanique des structures sandwiches réparées et de leur
processus d’endommagement. Les modèles par éléments finis développés dans ces travaux ont
été validés expérimentalement et des simulations paramétriques ont contribué à une meilleure
compréhension de l’influence des différents paramètres géométriques sur la résistance de la
réparation par patch interne.
v
Mots-clés : Structures sandwiches, Réparation collée, Simulation numérique, hors-autoclave,
Réparation en biseau, essais expérimentaux.
vi
Abstract
In service, aeronautical components made of composite materials and sandwich structures are
subject to type of damages that require repairs. Adhesively bonded repairs (scarf-scarf, step-
step or scarf-step) offer an excellent mechanical strength recovery for these composite
structures. However, the repair environment can be a significant challenge in terms of the
choice of geometrical parameters (scarf angle, addition of an overply), damage process
parameters and mechanical behavior under different loads.
This thesis presents both experimental and numerical investigations of the mechanical behavior
of internal patch repairs carried-out on Nomex honeycomb composite sandwich structures. The
skins use an out-of- autoclave woven fabric made of carbon-epoxy composite materials. In
order to determine the effect of different geometric parameters on the resistance of the internal
patch repair and to better understand its mechanical behavior and damage processes, a series
of mechanical tests under different loads (tensile, compression, bending) is conducted on the
repaired sandwich panels made with either plain weave or 8 harness satin textile composites.
Numerical simulations were carried out, in several stages, in order to determine the mechanical
behavior of the repair. First, a 2D model that assumes a linear elastic behavior of the adhesive
film was developed. This simple model allows to study the distribution of the stresses in the
adhesive joint for different configurations of rectangular patch repair. Then, the 2D model is
modified in order to account for the elastoplastic behavior of the adhesive film. The latter
allows to predict the mechanical behavior of a rectangular internal patch repair until rupture.
vii
Subsequently, a 3D model is developed to predict the mechanical behavior of circular internal
patch repairs under compressive loadings. This model takes into account the progressive
damage and failure of the woven fabric skins. The results of these numerical simulations are
validated by comparing them to experimental measurements. The finite element models that
account for the elastoplastic behavior law for the adhesive joint allow predictions of the
strength as well as the damage morphology of the repaired sandwich structures. A parametric
study has also been conducted in order to determine the influence of the geometrical design
parameters in the repair strength.
Processing and assessment of the mechanical performance of internal patch repairs on
sandwich structures is a complex task with multiple material and process parameters. In
general, this thesis contributes to a better understanding of the mechanical behavior of
adhesively bonded repaired sandwich structures and their damage process. The finite element
models developed in this work and validated experimentally have contributed through
parametric numerical simulations to an economical better understanding of the influence of
different geometric parameters on the strength and failure of internal patch repaired sandwich
panels.
Keywords: Honeycomb composite sandwich structures, Bonded repair, Progressive damage,
Step-scarf repair, Out-of-autoclave materials, Finite element analysis, and Experimental tests.
viii
Table of content
Résumé ................................................................................................................ iii
Abstract ................................................................................................................ vi
Table of content ................................................................................................ viii
List of Tables .................................................................................................... xiii
List of Figures .................................................................................................... xvi
Nomenclature ................................................................................................... xxii
Acknowledgements .......................................................................................... xxvi
Avant-Propos ................................................................................................. xxvii
Introduction ........................................................................................................... 1
Chapter 1. Literature Review ............................................................................. 8
1.1 A Review of Monolithic Composite Bonded Repair Design ..................................... 8
1.1.1 Composite Bonded Joint Repairs ........................................................................... 9
1.1.2 Analytical Methods .............................................................................................. 10
1.1.3 Finite Element Analysis Techniques ................................................................... 12
1.1.4 Failure Mechanisms of Composite Bonded Joint Repairs: Observations and
Modeling Process ............................................................................................................. 21
1.1.5 Review Summary ................................................................................................. 29
1.2 A Review of Honeycomb Sandwich Panel Bonded Repairs ................................... 29
1.2.1 Introduction .......................................................................................................... 30
1.2.2 State-of-The-Art Review of Sandwich Panel Repairs ......................................... 35
1.2.3 Concluding Remarks ............................................................................................ 44
ix
Chapter 2. Overview of the Problem and Research Focus .............................. 47
2.1 Rationale of the Thesis............................................................................................. 47
2.1.1 Assessment of the Mechanical Behavior of Honeycomb Sandwich Panels with
Bonded Repairs by Experimental Testing ....................................................................... 49
2.1.2 Development of Finite Element Models for Better Understanding and Accurate
Prediction of the Mechanical Behavior and Failure Modes of the Repaired Sandwich
Panels under Different Loadings ..................................................................................... 50
2.1.3 Validation of the Finite Element Models and Conduction of a Parametric Study
50
2.2 Methodology and Thesis Structure .......................................................................... 51
2.2.1 Methodology ........................................................................................................ 51
2.2.2 Chapters Presentation........................................................................................... 54
Chapter 3. Mechanical Characterization and Finite Element Study of
Monolithic Facesheets and Honeycomb Core .................................................... 56
3.1 Experimental Characterization of the Facesheet Materials ..................................... 57
3.1.1 Materials Description and Specimens Manufacturing ......................................... 57
3.1.2 Mechanical Testing of the Laminate Used for the Skins ..................................... 58
3.2 Mechanical Characterization of the Honeycomb Nomex Core ............................... 65
3.2.1 Out-of-Plane Compressive Tests ......................................................................... 66
3.2.2 In-Plane Tensile Tests .......................................................................................... 68
3.2.3 Nomex Tests Recapitulation ................................................................................ 69
3.3 Analytical and Finite Element Studies of the Facesheets Mechanical Behavior ..... 70
3.3.1 Classical Lamination Theory: Analytical Approach ............................................ 71
3.3.2 Finite element Analyses ....................................................................................... 73
3.4 Conclusion ............................................................................................................... 82
Chapter 4. Article 1: Mechanical Performance of Repaired Sandwich Panels:
Experimental Characterization and Finite Element Modelling .......................... 83
4.1 Introduction .............................................................................................................. 84
x
4.2 Experimental Work .................................................................................................. 88
4.2.1 Repaired Sandwich Specimen Preparation .......................................................... 88
4.2.2 Tensile tests procedure ......................................................................................... 91
4.2.3 Experimental Results ........................................................................................... 92
4.2.4 Damage Mode and Fractography Studies ............................................................ 94
4.3 Numerical Simulation .............................................................................................. 98
4.3.1 Model Description ............................................................................................... 98
4.3.2 Linear Elastic Numerical Model ........................................................................ 100
4.3.3 Non-linear Elastic Plastic Model ....................................................................... 102
4.3.4 Numerical Results and Discussion..................................................................... 106
4.4 Conclusions ............................................................................................................ 108
Chapter 5. Article 2: Parametric Study of Stepped-Scarf Bonded Joints in
Repaired Honeycomb Sandwich Composite Panels ......................................... 109
5.1 Introduction ............................................................................................................ 110
5.2 Finite Element Model Description ......................................................................... 114
5.2.1 Model Geometry and Material System Description .......................................... 114
5.2.2 Boundary Conditions and Finite Element Mesh Details.................................... 116
5.2.3 Materials Models ............................................................................................... 117
5.3 Parametric Study .................................................................................................... 118
5.4 Results .................................................................................................................... 120
5.5 Discussion .............................................................................................................. 131
5.6 Conclusions ............................................................................................................ 135
Chapter 6. Article 3: Evaluation of the mechanical performance of repaired
composite sandwich structure using different mechanical tests ....................... 138
6.1 Introduction ............................................................................................................ 139
6.2 Experimental Work ................................................................................................ 143
6.2.1 Materials ............................................................................................................ 143
6.2.2 Repair Procedure ................................................................................................ 143
xi
6.2.3 Specimen Preparation and Test Procedure ........................................................ 144
6.2.4 Results and Discussion ...................................................................................... 151
6.3 Finite Element Analysis ......................................................................................... 161
6.3.1 Model Description ............................................................................................. 161
6.3.2 Model Results .................................................................................................... 164
6.4 Conclusion ............................................................................................................. 166
Chapter 7. Article 4: Experimental and Numerical Studies of Stepped-Scarf
Circular Repair in Composite Sandwich Panels ............................................... 169
7.1 Introduction ............................................................................................................ 171
7.2 Experimental Work ................................................................................................ 175
7.2.1 Objective and Methodology ............................................................................... 175
7.2.2 Specimen Preparation ........................................................................................ 176
7.2.3 Edgewise Compressive Tests ............................................................................. 179
7.2.4 Four-Point Bend tests ......................................................................................... 181
7.3 Numerical Simulation ............................................................................................ 185
7.3.1 Finite Element Model Description ..................................................................... 185
7.3.2 Failure Criteria and Damage Evolution ............................................................. 188
7.3.3 Results and Discussions: Edgewise Compressive Tests .................................... 191
7.4 Conclusion ............................................................................................................. 195
Chapter 8. Conclusions and Perspectives ...................................................... 197
8.1 Thesis Conclusions ................................................................................................ 197
8.2 Thesis Original Contributions ................................................................................ 201
8.3 Recommendations for Future Work....................................................................... 204
References ......................................................................................................... 206
Appendix A. Mechanical performance of the 8HS honeycomb sandwich panels
........................................................................................................................... 212
A.1 Tensile Tests on Pristine and Repaired 8HS Honeycomb Sandwich Panels ......... 212
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Specimens Dimensions and Test Set-up ............................................................ 213
Test Results for the Pristine 8HS Honeycomb Sandwich Panels ...................... 214
Test Results for the 2D Repaired 8HS Honeycomb Sandwich Panels .............. 214
Strength Recovery of the 3°-Repaired Sandwich Panels ................................... 217
A.2 Compressive Tests on 8HS Honeycomb Sandwich Panels ................................... 218
Compressive Tests on Pristine and 2D Repaired Honeycomb Panels ............... 219
A.2.1.1 Compressive Tests on the Pristine 8HS Honeycomb Sandwich Panels ............ 219
A.2.1.2 Compressive Tests on the 2D Repaired 8HS Honeycomb Sandwich Panels .... 221
A.2.1.3 Recapitulation and Strength Recovery of the 8HS Repaired Sandwich Panels. 222
Compressive Tests on 3D Repaired and Open-Hole 8HS Honeycomb Panels . 224
A.3 Flexure Tests on Pristine and 2D Repaired 8HS Honeycomb Sandwich Panels ... 227
Long-Beam Flexure Tests .................................................................................. 227
Tests Results and Interpretation ......................................................................... 229
A.4 Results Validation .................................................................................................. 232
xiii
List of Tables
Table 1-1 Parameters effects on the peel and shear stresses [21] ........................................ 17
Table 1-2 Issues and aspects studied in the literature for composite bonded repairs ........... 29
Table 1-3 Structural efficiency of sandwich panels in terms of weight [41] ....................... 31
Table 1-4 Sandwich panels component materials used in the literature .............................. 45
Table 1-5 Repair configuration, process and cure methods for sandwich panel repairs used
in the literature ......................................................................................................................... 46
Table 1-6 Mechanical characterization and non-destructive inspection of sandwich panel
repairs used in the literature ..................................................................................................... 46
Table 1-7 Finite element model types used in the literature for sandwich honeycomb panels
.............................................................................................................................. 46
Table 3-1 Materials properties from Cytec [59] ................................................................... 57
Table 3-2 Statical analysis - tensile tests .............................................................................. 64
Table 3-3 Statical analysis - compressive tests .................................................................... 65
Table 3-4 Mechanical properties for the ECA-R Nomex core (from [63]).......................... 66
Table 3-5 Compressive mechanical properties for the over-expanded Nomex core ........... 67
Table 3-6 Tensile elastic modulus in the L-and W-directions for the over-expanded Nomex
core .............................................................................................................................. 69
Table 3-7 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R 4.8
64) .............................................................................................................................. 70
Table 3-8 Composite materials elastic properties ................................................................ 72
Table 3-9 Comparison between analytical and experimental results ................................... 73
Table 3-10 Predicted and measured elastic modulus of the quasi-isotropic laminate ........ 77
Table 3-11 Mechanical properties used for the PW composite material ........................... 80
Table 3-12 Comparison between the experimental data and the finite element prediction 80
Table 4-1 Test matrix. .......................................................................................................... 92
xiv
Table 4-2 Comparison of the ultimate stress between the sandwich skin and a [(+45/-45)/
(0/90)/ (-45/+45)/ (90/0)]2s quasi-isotropic laminate made from the same PW prepreg [74] .. 95
Table 4-3 Mechanical properties of the plain weave material. ............................................ 99
Table 4-4 Mechanical properties of the FM300-2M adhesivea. ........................................... 99
Table 4-5 Mechanical properties of the Nomex honeycomb core ..................................... 100
Table 4-6 Stiffness prediction of pristine panels. ............................................................... 101
Table 4-7 Hardening data input. ......................................................................................... 106
Table 5-1 Mechanical properties of the plain weave composite material .......................... 117
Table 5-2 Mechanical properties of the FM300-2M adhesive ........................................... 118
Table 5-3 Mechanical properties of the Nomex honeycomb core ..................................... 118
Table 5-4 Parametric model details .................................................................................... 119
Table 5-5 Baseline model values........................................................................................ 120
Table 6-1 Test matrix for different experimental tests ....................................................... 144
Table 6-2 Summary of the compressive test results ........................................................... 154
Table 6-3 Summary of the tensile test results .................................................................... 156
Table 6-4 Summary of the flexure test results ................................................................... 157
Table 6-5 Elastic material properties of the plain weave carbon-epoxy ply ...................... 163
Table 6-6 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R 4.8
64) ............................................................................................................................ 163
Table 6-7 Mechanical properties of the hexagonal Nomex honeycomb core (ECA 3.2 96) ...
............................................................................................................................ 164
Table 6-8 Mechanical properties of the FM300-2M adhesive film ................................... 164
Table 7-1 Mechanical properties of the plain weave composite material (CYCOM 5320
T650 PW). ............................................................................................................................ 178
Table 7-2 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R 4.8
64). ............................................................................................................................ 178
Table 7-3 Mechanical properties of the hexagonal Nomex honeycomb core (ECA 3.2 96) ...
............................................................................................................................ 179
Table 7-4 Mechanical properties of the FM300-2M adhesive [76]. .................................. 179
xv
Table 7-5 Test matrix. ........................................................................................................ 181
Table 7-6 Test results for different sandwich panels configuration. .................................. 183
xvi
List of Figures
Figure 1-1 Common configurations of bonded repair joints, 2D geometries .................... 10
Figure 1-2 Failure mechanisms of a bonded joint ............................................................. 22
Figure 1-3 A tension-loaded 2D scarf joint used in the literature [31] .............................. 22
Figure 1-4 Failure morphology of a low scarf repair joint angle under tensile load [31] . 24
Figure 1-5 Failure paths observed in the static tensile 2°-scarf repaired joints under
different environmental conditions [16] .................................................................................. 24
Figure 1-6 Failure morphology of a circular patch repair: (a) top surface (b) bottom surface
(adapted from [30]) .................................................................................................................. 25
Figure 1-7 Cohesive zone models’ presentation: (a) triangular law, (b) trapezoidal law [20].
.......................................................................................................................... 27
Figure 1-8 Nomenclature used to describe the sandwich panel geometric characteristics 31
Figure 1-9 Different failure modes of a sandwich panel [43]. .......................................... 35
Figure 1-10 Typical scarf-type repair procedure of a honeycomb composite sandwich panel
.......................................................................................................................... 36
Figure 1-11 Scarf-type repair patches on honeycomb sandwich panel ............................... 38
Figure 2-1 Repair configurations in sandwich honeycomb panels .................................... 49
Figure 2-2 Flowchart of the research methodology ........................................................... 51
Figure 2-3 Longitudinal-cross section modeled with 2D model ....................................... 53
Figure 2-4 Circular 3D model geometry ........................................................................... 53
Figure 3-1 Fiber architecture pattern for a) an 8HS fabric and b) a PW fabric (adapted
from[60]) .......................................................................................................................... 57
Figure 3-2 Vacuum bag arrangement and cure cycle used for the quasi-isotropic laminates
.......................................................................................................................... 59
Figure 3-3 Micrographs of PW and 8HS laminate cross-sections after cure .................... 60
Figure 3-4 CLC set-up and specimen configuration.......................................................... 61
xvii
Figure 3-5 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW
specimen tested in tension ....................................................................................................... 62
Figure 3-6 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]s 8HS
specimen tested in tension ....................................................................................................... 62
Figure 3-7 Typical failure for specimens tested in tension in the x- and y-directions ...... 63
Figure 3-8 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW
specimen tested in compression in the x-direction .................................................................. 63
Figure 3-9 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]s 8HS
specimens tested in compression in the x-direction ................................................................. 63
Figure 3-10 Typical failure mode for specimens tested in compression in the x-direction 64
Figure 3-11 Nomenclature and dimensions of a ECA-R unit cell (4.8 mm) ....................... 66
Figure 3-12 Compressive test set-up ................................................................................... 67
Figure 3-13 Typical compressive stress-strain curve .......................................................... 67
Figure 3-14 Specimen configuration and tensile test set-up ................................................ 68
Figure 3-15 Typical tensile stress-strain curves in the ribbon (L) and transverse (W)
directions .......................................................................................................................... 70
Figure 3-16 Geometry of studied and simplified specimen (not to scale) ........................... 74
Figure 3-17 Changes in Stiffness matrix to respect modelling convention ......................... 75
Figure 3-18 Boundary conditions for the 2D laminate tensile test (not to scale) ................ 75
Figure 3-19 Comparison of stress-strain curves between the experiment and the finite
element model for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW tested in tension in the x-
direction .......................................................................................................................... 81
Figure 3-20 Comparison of stress-strain curves between the experiment and the finite
element model for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW tested in compression in the x-
direction .......................................................................................................................... 81
Figure 4-1 Parent panel dimension (not to scale). ............................................................. 89
Figure 4-2 1D scarf/step repair configuration (not to scale). ............................................. 91
Figure 4-3 Tensile test set-up. ........................................................................................... 93
xviii
Figure 4-4 Axial load-strain curves obtained for the pristine and 3-repaired sandwich
specimens (strains measured by DIC on the tool facesheet). ................................................... 93
Figure 4-5 Comparison of the axial load-strain curves obtained on both facesheets of the
sandwich specimens. ................................................................................................................ 94
Figure 4-6 Tensile failure load of the pristine and repaired sandwich specimens............. 94
Figure 4-7 Failure mode of pristine panels. ....................................................................... 96
Figure 4-8 Failure mode for the 3°-repaired sandwich panels. ......................................... 96
Figure 4-9 Micrograph of the cross-section of the (a) pristine specimen, (b) repaired
sandwich specimen before testing. .......................................................................................... 97
Figure 4-10 Micrograph of the 3°-repaired sandwich specimen cross-section after failure....
.......................................................................................................................... 97
Figure 4-11 Description of the boundary conditions. .......................................................... 99
Figure 4-12 Line and local coordinate system used to extract peel and shear stresses ..... 101
Figure 4-13 Shear stress distribution along the bondline. ................................................. 102
Figure 4-14 Peel stress distribution along the bondline..................................................... 102
Figure 4-15 Finite element prediction versus experiment results for the 3°-repaired sandwich
panels. ........................................................................................................................ 107
Figure 4-16 Failure load and efficiency (η= 𝑃𝑟𝑒𝑝𝑎𝑖𝑟𝑓𝑃𝑢𝑛𝑑𝑎𝑚𝑎𝑔𝑒𝑑𝑓𝑥100) for different
scarf-step angles. .................................................................................................................... 107
Figure 5-1 Configuration of the double scarf-stepped repair joint (not to scale). ........... 115
Figure 5-2 Symmetric cross-section of the double scarf-stepped repaired sandwich panel
(not to scale). ........................................................................................................................ 116
Figure 5-3 Line and local coordinate system to extract peel and shear stresses in the
adhesive joint. ........................................................................................................................ 119
Figure 5-4 Shear and peel stress distributions along the adhesive bondline for different
scarf angles. ........................................................................................................................ 121
Figure 5-5 Repair failure stress for different scarf angles. .............................................. 122
Figure 5-6 Shear and peel stress distributions along the adhesive bondline as a function
overlap length Lo (3°-4-ply skin model). ............................................................................... 126
xix
Figure 5-7 Determination of the minimal overply overlap length ................................... 127
Figure 5-8 Repair strength prediction as function of the overlap length, Lo (3°-4-ply skin
model). ........................................................................................................................ 127
Figure 5-9 Failure morphology of a specimen with an overlap length, Lo=10. .............. 127
Figure 5-10 Shear and peel stress distributions along the adhesive bondline as a function of
number of skin plies, N (α=3o)............................................................................................... 130
Figure 5-11 Repair strength prediction as function of the number of skin plies, N (α=3°). ....
........................................................................................................................ 131
Figure 5-12 Map of the failure stress as a function of the scarf angle and number of plies, N.
........................................................................................................................ 134
Figure 5-13 Variation of the failure stress as a function of the overply and number of skin
plies, N (α=3°). ...................................................................................................................... 134
Figure 6-1 Parent panel dimension (not to scale) ............................................................ 145
Figure 6-2 2D stepped-scarf repair configuration ........................................................... 145
Figure 6-3 Specimen geometry (not to scale) .................................................................. 147
Figure 6-4 CAI fixture system used for the edgewise compressive tests ........................ 147
Figure 6-5 Location of strain gages (not to scale) ........................................................... 148
Figure 6-6 Micrograph of the repair cross-section before testing ................................... 148
Figure 6-7 Tensile test set-up. .............................................................................................. 149
Figure 6-8 Four-point bend test fixture and specimen configurations (not to scale) ....... 150
Figure 6-9 Typical force versus strain curves for pristine and 3°-repaired sandwich
specimens tested in compression ........................................................................................... 152
Figure 6-10 Force-strain curves obtained using different strain measuring instruments for
pristine and 3°-repaired sandwich specimens tested in compression .................................... 153
Figure 6-11 DIC measurement: out-of-plane displacement of 3°-repaired sandwich
specimen tested in compression at failure ............................................................................. 153
Figure 6-12 Micrograph of the repair cross-section after failure of 3°-repaired sandwich
specimen tested in compression ............................................................................................. 154
xx
Figure 6-13 Typical axial load-strain curves for the pristine and 3°-repaired sandwich
specimens tested under tension .............................................................................................. 156
Figure 6-14 Typical stress versus strain curves for pristine and 3°-repaired sandwich beams
tested under four-point bending ............................................................................................. 157
Figure 6-15 . Failure mode of a 3°-repaired sandwich beam tested under four-point bending
(repair in tension) ................................................................................................................... 157
Figure 6-16 Comparison of the failure stress of the pristine panels obtained from different
loading types. ........................................................................................................................ 160
Figure 6-17 Comparison of the failure stress of the 3°-repaired panels obtained from
different loading types. .......................................................................................................... 160
Figure 6-18 Studied longitudinal cross-section of the repaired specimens ....................... 162
Figure 6-19 Model geometry and boundary conditions for the four-point bend test ........ 163
Figure 6-20 Mesh details of the adhesive bondline ........................................................... 163
Figure 6-21 Numerical predictions versus experimental results for 3°-repaired sandwich
specimens under different load cases. .................................................................................... 165
Figure 6-22 Deformation and failure mode for a 3°-repaired beam tested under four-point
bending (repair in compression) ............................................................................................ 166
Figure 7-1 Stepped-scarf repair zone cross-section (not to scale). .................................. 178
Figure 7-2 Compressive test fixture and strain gages location. ....................................... 181
Figure 7-3 Specimens configuration and four-point bending test fixture. ....................... 183
Figure 7-4 Stress-strain curves for the pristine sandwich beams. ................................... 184
Figure 7-5 Stress-strain curves for the 3° repaired sandwich beams. .............................. 184
Figure 7-6 Failure morphology of the pristine and the 3°-repaired sandwich beams under
four-point bending. ................................................................................................................ 185
Figure 7-7 Failure stress of the pristine and 3° repaired panels under four-point bending. ..
........................................................................................................................ 185
Figure 7-8 Mesh details of the honeycomb sandwich panels. ......................................... 187
Figure 7-9 Mesh refinement details of the 3°-repaired panel .......................................... 188
Figure 7-10 Boundary conditions applied in the finite element model. ............................ 188
xxi
Figure 7-11 Finite element prediction versus experiment results for composite sandwich
panels ........................................................................................................................ 193
Figure 7-12 Failure mode for the tested composite sandwich panels. ............................... 194
Figure 7-13 Predicted failure morphology for the three panel configurations. ................. 194
xxii
Nomenclature
List of Latin symbols
Loverlap: Overlap Length
L: Total Length of the Specimen
F: Applied Force
A: Section Area
E: Elastic Modulus
G: Shear Modulus
S: Standard Deviation
N: Number of Plies
t: Total Thickness of the Specimen
w: Total Width of the Specimen
tf: Thickness of the Facesheet
ta: Thickness of the Adhesive Film
tp: Thickness of the Ply
tc: Core Thickness
xxiii
List of Greek symbols
σi: Stress (i=x, y)
ν: Poisson’s ratio
α: Scarf Angle
ρ: Density
List of acronyms
RTM: Resin Transfer Molding
C.V: Coefficient of Variation
CLT: Classical Lamination Theory
CFRP: Carbon Fiber Reinforced Plastic
U.D: Unidirectional
RT: Room Temperature
FE: Finite element
OOA: Out-of-Autoclave
PW: Plain Weave
8HS: Eight Harness Satin
DIC: Digital Image Correlation
CZM: Cohesive Zone Model
xxiv
TAST: Thick Adherend Shear Test
CAI: Compression after Impact
S8R: Eight-Node Reduced Integration Shell Elements
AGARD: Advisory Group for Aerospace Research & Development
BVID: Barely Visible Impact Damage
xxv
To my parents, sisters and brothers
xxvi
Acknowledgements
First and foremost, I would like to express my deepest gratitude to Professors Marie-Laure
Dano and Augustin Gakwaya, my research supervisors, for providing me with continuous
opportunities to grow as a young researcher. Their constant support and constructive advices
made these years at Laval University rich in terms of technical learning and personal
development. Thank you for all your support Marie-Laure and Augustin.
Many thanks to Charles-Olivier Amyot for his time and help to ensure the manufacturing and
testing of the sandwich panels. Many thanks also to Mathieu Pouliot and Jonathan Guy-Larose.
I am very thankful to the industrial partners for sharing their expertise in composite repairs,
especially David Wilson, Hasan Salek, Isabelle Paris from Bombardier Aerospace and Étienne
Bélanger from L3-Mas. Thank you for reviewing my papers.
This project was made possible by the financial support, materials provision, and access to
equipment from the Consortium for Research and Innovation in Aerospace in Quebec
(CRIAQ); the Natural Science and Engineering Research Council (NSERC), the National
Research Council Canada (NRC/CNRC), Université Laval, École Polytechnique de Montréal
McGill University, Bombardier Aerospace and L-3 MAS.
xxvii
Avant-Propos
Ce travail présente une thèse par articles comprenant quatre articles qui sont soit publié, accepté
pour publication ou soumis. Ces articles sont :
Article 1 intitulé “Mechanical performance of repaired sandwich panels: Experimental
Characterisation and finite element modeling’’ a été soumis en décembre 2016 au
journal Sandwich Structures and Materials et publié en mai 2017. L’auteur principal
pour cet article est Emna Ghazali et les co-auteurs sont : Marie-Laure Dano, Augustin
Gakwaya et Charles-Olivier Amyot.
Article 2 intitulé “Parametric study of stepped-scarf bonded joints in repaired
honeycomb sandwich composite panels’’ a été soumis au Journal of Adhesion en
novembre 2017. L’auteur principal pour cet article est Emna Ghazali et les co-auteurs
sont: Marie-Laure Dano et Augustin Gakwaya.
Article 3 intitulé “Evaluation of the mechanical performance of repaired composite
sandwich structure using different mechanical tests’’ a été soumis au Journal of
Adhesion & Adhesives en décembre 2017. L’auteur principal pour cet article est Emna
Ghazali et les co-auteurs sont: Marie-Laure Dano, Augustin Gakwaya et Charles-
Olivier Amyot.
Article 4 intitulé “Experimental and numerical studies of stepped-scarf circular repairs
in composite sandwich panels’’ a été soumis en juillet 2017 au Journal of Adhesion &
xxviii
Adhesives et accepté pour publication avec corrections mineures en octobre 2017.
L’auteur principal pour cet article est Emna Ghazali les co-auteurs sont: Marie-Laure
Dano, Augustin Gakwaya et Charles-Olivier Amyot.
Les versions intégrées dans cette thèse sont les versions publiées ou soumises des articles.
La candidate a effectué les travaux expérimentaux et numériques présentés dans ces articles à
quelques exceptions près indiqués ci-dessous :
Article 1: Mathieu Pouliot, étudiant stagiaire, a aidé à la préparation des éprouvettes.
Charles-Olivier Amyot, professionnel de recherche a aidé dans les différents tests
mécaniques.
Article 3 : Jonathan Guy La rose et Éloïse Dol, étudiants stagiaires ont aidé à la
fabrication et aux tests mécaniques de la flexion 4-points avec une étroite participation
de Charles-Olivier Amyot pour la conception du montage de flexion.
Article 4 : Charles-Olivier Amyot a aidé dans les tests de compression.
1
Introduction
Although advanced composite materials and especially honeycomb sandwich structures have
been traditionally used in aerospace applications, they have gained more popularity in high-
performance structural design in the last years. The diversity of the types of reinforcements
(carbon, glass, graphite, etc.), resins and associated manufacturing processes (autoclave, RTM,
out-of-autoclave, etc.) shows that the use of these materials (monolithic or sandwich structures)
is expanding. Their success is due to the various advantages they can offer compared to metals:
good fatigue performance, good resistance to corrosion, high-strength-to-weight ratio (light-
weight-to-stiffness ratio) etc. However, independent of the airframes materials, structural
damage inevitably occurs while in service as a consequence of accidental contact with ground
service vehicle, in-flight hailstones, bird strikes or lightning strikes that may cause critical
damages. Hence following reference [1], “the maintenance and repair of these components are
vital to ensure that the performance of these composite components remain the same as they
were initially designed”( p.919). The damage extent determines whether the component needs
to be repaired or replaced. Moreover, because of time constraint issues, repairs must be
performed as quickly as possible so that the aircraft can be returned into service as soon as
possible. After inspection, maintenance procedure will depend on damage extent. If damage is
minor (i.e., it does not affect the structural integrity of the part), then it is classified as an
allowable damage and only requires a cosmetic repair. However, when damage exceeds the
2
allowable damage size, a structural repair is needed in order to restore the initial carrying
capacities of the structure. Finally, for damage larger than the repairable damage limit size, if
an appropriate repair cannot be substantiated, the component has to be replaced. So, one of the
main challenges facing the aerospace industry with composite materials (monolithic and
sandwich) is structural repair. With the increase of the number of aircraft primary structure
components made of composite materials (either monolithic or honeycomb sandwich), it has
become necessary to develop repair methods that will restore the component’s original design
strength without compromising its structural integrity [2]. It is therefore essential to have
robust, reliable and reproducible procedures related to structural repair to restore the strength
and integrity of damaged composite and sandwich structures. However, with existing repair
technologies, structural repairs present several scientific challenges, especially with primary
structures. To repair damaged structural components, two main methods are typically
considered: bolted repairs and bonded repairs, and bonded repairs are divided into external
bonded repair patches and scarf-type bonded repair patches. Bolted repairs increase
significantly the weight of the component. Also, fasteners offer non-negligible stress
concentrations around the bolt holes. According to [1], depending on the type of damage
sustained, “different repair techniques have been developed to address each specific case’’
(p.900-904). To repair a wide range of cracks or damage to aircraft components and structures,
externally bonded composite repair patches have been shown to be effective [3]. They were
originally used for the repair of military aircraft, but have since been used on civil aircraft.
Traditionally, repairs on metallic aircraft structures were performed using bolted joints,
3
however bonded repairs are the most common repair technique used with composite materials
[4]. The advantages of utilizing bonded composite repairs [5] include:
High resistance to damage by cyclic loads, immunity to corrosion, and high formability that
allows easy forming into complex shapes.
Compared to bolted repairs, bonded repairs offer an alternative repair method that can
effectively reduce the introduction of unwanted stress risers caused by the fasteners used
in a bolted repair, which can severely hinder the performances of the repair [6].
Another disadvantage of using a bolted repair is the likelihood of damaging the surrounding
material while drilling fastener holes.
Composite materials can delaminate from improper hole drilling procedures and
from excessive heat generated from the hole drilling.
Hence to reduce the possibility of thermal delamination, diamond tipped cutting
wheels are utilized in the surface grinding equipment, together with coolant that
is used during the partitioning process.
Due to the advantages from utilizing bonded repairs, the Composite Aircraft Field Repair
Method (CAFRM) is being developed as a bonded field repair. There are two types of bonded
repairs commonly used to repair structural damage.
The first type of bonded repair is an external repair patch that can recover most of the
component’s strength. It has the advantage of being easy to perform and does not require a
4
large amount of time to complete [6]. This makes it a good candidate for a field repair
method.
The effectiveness of bonded external patch repairs depends on several design
parameters that play a vital role. These include in particular, the patch size, patch
shape, materials used, patch taper, patch fiber orientation, and curing
temperatures of the patch [6]. In order to ensure that the stresses induced into
the adhesives are within the design limits of both the material and the operating
envelope of the aircraft structure, care must be taken during the design phase of
these patches.
Most of these parameters are defined by the manufacturer’s Structural Repair
Manual (SRM) for the specific aircraft structure being repaired.
The second type of bonded repair is a scarf-type patch. Compared to external patches,
because of the matching of the repair plies to the plies in the original structures, scarf-type
patches provide higher stiffness. Moreover, the amount of stress risers in a scarf-type patch
repairs are also lower than in external patch repairs.
By matching the neutral axis of the repair patch to the original structure, scarf-
type patch repairs are more efficient in load transfer due to the reduced load
eccentricity [7].
However, aside from the advantages a scarf-type patch repair has over an external patch repair,
scarf-type patch repairs have also some disadvantages:
5
They require a large amount of original material to be removed in order to
maintain a small taper angle.
The placement of the repair plies must be accurately laid up in the repair joint
to the same orientation and order as the original structure. “The accurate
placement of repair plies can be very challenging and the risks of errors are
very high” [1].
The performance of the scarf-type patch can greatly depend on the curing
method utilized to cure the repair. “Repairs cured using different methods
compared to the original structure can greatly affect the strength of the repairs
and cause a mismatch between the original structure and the repair patch’’.
Finally, the adhesives flow under the scarf-type repair patch during curing can
be hard to control, causing the adhesives to accumulate in the bottom of the
patch thus creating a non-uniform bondline.
Due to all these characteristics, a scarf-type repair patch can be:
“Very time consuming and highly dependent on the skill level of the maintenance technician
due to the requirement of accurately removing original materials from the structure and of
precisely replacing the removed materials with new composite materials. Scarf-type repair
patch can thus hardly be considered as candidate for bonded field repair’’.
6
With the above challenges in mind, the authors in [7] then recommend that: “if a scarf type
repair is to be performed on a part that is not considered to be a lightly loaded component, the
scarf-type patch repair should be performed at a repair facility where equipment such as an
autoclave is available in order to produce repaired aircraft parts that have the same part
strength as the original structure”.
In this project, we are concerned with out-of-autoclave composites, and we will try to develop
bonded repair techniques appropriate for out-of-autoclave (OOA) woven composites with the
ultimate goal of setting up a field repair technology for this kind of composites.
This thesis research work is part of the CRIAQ COMP-507 project, which brings together
several partners from industry (BA, L-3Mas), from academics (Laval, McGill, Polytechnique)
and from government Laboratory (NRC-CNRC) for the development of reliable repair methods
and analytical and numerical tools for the repair of composite structures and primary sandwich
panels for aeronautical applications. Its objective is to propose a numerical and experimental
techniques to study the behavior of bonded repair methodology, specifically adapted to primary
sandwich composite structures.
Thesis Organization
The research work achieved in this thesis is organized through five body chapters as follows:
In chapters 1 and 2 a state of the art literature review related to bonded repair joints on
composite laminate structures is first presented. This is followed by a review of experimental
work and finite element techniques employed for modeling different repair joints for
monolithic composites. The chapter ends with review of existing techniques for bonded repairs
7
of composite sandwich structures and associated mechanical testing and finite element
modeling techniques. Finally, the justification of the work to be done and detailed objectives
and methodology of the present work are presented, and the thesis work contributions are then
highlighted.
In chapter 3, the characterization of the sandwich panel’s constituents is presented. Here, in-
plane tension and compression tests as well as out-of-plane tests for woven facesheets and
Nomex core are considered followed by the development of finite element simulation
methodology validated by the simulation of experimental tests.
In chapter 4, the experimental and numerical studies of rectangular (2D) scarf patch repairs of
sandwich panels are presented.
In chapter 5, focus is centered on the parametric study of the effect of different geometric
parameters on the strength recovery of the repaired sandwich panels under tensile loads.
In chapter 6, experimental and numerical investigations on 2D repaired sandwich panels tested
under edgewise compression and four-point bending loads are presented.
In chapter 7, experimental and numerical studies of circular scarf patch repairs are considered.
First compressive and four-point bend tests are performed to determine the behavior of the
repaired sandwich panel and beams. This is followed by the development of 3D finite-element
models with a progressive damage and failure in order to predict the stiffness and failure mode
of the repaired panels.
The thesis work then ends with a conclusion in Chapter 8 that summarizes the contributions
from this research, and gives some recommendations and perspectives for future work.
8
Chapter 1.
Literature Review
The objective of this chapter is to present a state of the art review of current practices in
composite bonded repairs technology in order to identify key issues that require further
investigations and that may form part of the core of the research work to be carried out in this
project. This chapter begins by reviewing the current design guidelines for composite bonded
repairs and then emphasizes on the main challenges associated with scarf bonded repairs,
including the geometric parameters effects on the strength recovery, the optimum taper angle
and the numerical simulation of the repair joint mechanical behavior. The second part of the
chapter then focuses on the principal theme of the thesis related to the major difficulties
encountered with bonded repairs of honeycomb sandwich panels. Finally, the chapter ends by
identifying areas where further investigations are needed.
1.1 A Review of Monolithic Composite Bonded Repair Design
This section reviews methods for designing adhesively bonded repair patches for monolithic
composites. Firstly, an overview of composite internal bonded repair techniques is presented.
Here, experimental works and observations of the failure modes of scarf joints and scarf repairs,
design improvements such as scarf angle optimization, addition of an overply and stacking
sequence are discussed. Secondly, analytical methods to study the stress distribution and the
resistance of the repair are presented. This is followed by a discussion of finite element analyses
9
methods developed for predicting the behavior of composite adhesively bonded repair joints.
Here, both 2D and 3D developed finite element models are discussed. Finally, the failure
mechanics of bonded joints are reviewed.
1.1.1 Composite Bonded Joint Repairs
Bonded joint repairs have significant advantages over fastened or bolted repair joints,
especially for aircraft composite structures. These are expressed in term of high strength-to-
weight ratio, better resistance to corrosion and absence of high stress concentrations at
fastener's holes [8]. The common configurations of bonded joints [9], applied to patch repairs
in aerospace structures, are illustrated in Figure 1-1: single and double lap joints, scarf-scarf
joints and step-step joints. Scarf and stepped bonded joints are typically preferred over double
lap (external patches) due to their higher strength recovery [10].
Scarf Joints
Scarf joints are also called smooth tapered joints or tapered-tapered joints. This type of joint
has many advantages over single and double lap joints such as the reduction in shear and peel
stresses. The stress distribution of scarf joints between identical adherends is almost uniform
and these joints have a higher strength recovery in comparison with other adhesive joints. So,
for these reasons, such joints are used for highly loaded structures. However, the repair patch
in scarf joints cannot be co-cured and need to be pre-cured before being bonded to the parent
structure.
10
Figure 1-1 Common configurations of bonded repair joints, 2D geometries
Stepped Joints
Stepped joints are used as alternative to scarf joints because they are easier to manufacture and
can be co-cured with the adhesive bondline. In theory, with an infinite number of steps, a
stepped joint becomes a scarf joint. While the strength of a scarf joint increases as the angle
decreases, however for a stepped joint with a fixed number of steps, the strength will not
continue to increase indefinitely as the angle decreases. Moreover, material removal for stepped
repairs is a more complex operation than scarfing and proper stepping requires expensive
grinding equipment [11].
1.1.2 Analytical Methods
Different approaches have been used to design bonded joint repairs. Analytical methods were
used by different authors [12,13] in the early 1970’s to study the behavior of scarf joints. Over
the years, as the capability of finite element packages increased, different finite element models
were developed to study the complex behavior of composite bonded joints and to improve the
analytical solutions. The most important points that were improved are:
• The prediction of the peel and shear stresses in the bonded joint,
11
• The modelling of extra plies used to reinforce the bonded structure,
• The modelling of a three-dimensional patch, etc.
The first research published on the use of analytical methods to study the behavior of scarf
joints were studies done by Hart-Smith [12] and Erdogan and Ratwani. [13]. In both studies, a
complete analytical method for the behavior of scarf joints used to repair composite aircraft
structures is developed. Here, the adhesive was modeled as a series of tension and shear springs
and both identical and dissimilar adherends were used.
Hart-Smith [12] showed that the ratio of the peak shear stress concentration at the stiffer
adherend tip relative to the average shear stress across the joint was observed to approach the
ratio of the adherend Young’s modulus. He observed that dissimilarities between adherend
materials contribute to the non-uniformity in the bondline shear and peel stresses. His model
also proposes a simple method for accounting of the non-linearity in the adhesive at high loads.
He was also able to suggest that the integrity of the scarf joint tips was important in maintaining
the overall integrity of the joint.
Erdogan and Ratwani [13] developed a model that was slightly more complete than Hart-Smith
[12]. In this model, they considered both the mechanical behavior of the adhesive in both shear
and normal directions to the bondline. Whereas Hart-Smith [12] assumed that the normal stress
was negligible, Erdogan and Ratwani [13] were also able to deduce from their studies that the
stress distribution in the bondline was not uniform between composite adherend. A stress
concentration in the adhesive was observed near the stiffer plies that correspond to 0°-ply
12
orientations. This was explained by the fact that load transfer through the joint occurs in these
particular locations.
Harman and Wang [14] developed an analytical technique based on the original equations
developed by Erdogan and Ratwani [13] to optimize the shape of scarf joints and to reduce the
shear and peel stress concentration in the adhesive bondline. Analytical equations were used to
conduct a sensitivity analysis to determine the optimal scarf angle for similar and dissimilar
composites adherends. The developed technique is based on a linear variation of the scarf angle
that generates a scarf profile for a given adherend modulus ratio. Harman and Wang showed
the dependency of the adhesive bondline stress distribution to the ply orientation and they
validated their analytical technique through finite element analyses.
1.1.3 Finite Element Analysis Techniques
Due to the limitation of the analytical methods to produce the singularities that a bonded
repaired joint can have, finite element analysis techniques were developed. The finite element
based numerical studies of adhesively-bonded joint repairs (internal or external patch)
considered analyses of either two-dimensional (using plane strain or plane stress assumptions)
or three-dimensional configurations. Many studies have been conducted on bonded joint
repairs of monolithic laminates.
Two-Dimensional (2 D) Analyses
Charalambides et al. [15] performed a two-dimensional numerical analysis to determine the
failure and strength of adhesively-bonded repairs on composites structures. The numerical
predictions were compared to experimental results [16] performed in unageing and ageing
13
conditions (hot/wet conditions). The adhesive bondline was modelled using a linear elastic and
a linear elastic-plastic material models. The composite plies were modelled using two different
approaches. First, the composite structure was assumed to be a homogeneous orthotropic
material. Then, each ply of the structure was modelled as an anisotropic material. Three
different failure modes in 2°-scarf repairs were observed: failure in the adhesive layer, failure
induced from delamination initiating at the corner of the overlap ply and tensile failure of the
composite adherend. Failure loads were compared with previously published experimental
work [16] and the results were found to be in good agreement for green (unaged) repaired
specimens. However, the predicted failure load, associated with delamination, did not occur
for the conditioned repair joints and no conclusion was established by the authors.
In a second approach, Campilho et al. [17–20] have conducted a lot of work to study the
mechanical behavior of external and internal bonded patch repairs. They use a two-dimensional
(2D) finite element model including a cohesive zone element and progressive damage to assess
the strength of external and adhesive repaired patch of Carbon Fiber Reinforced Plastic (CFRP)
under tensile and compressive loads. A mixed-mode cohesive damage model, for ductile
adhesives, was used in the analyses to simulate the adhesive layer behavior.
In [17], Campilho et al. published a study related to the mechanical behavior of single and
double-lap repair joints under tensile loading. A 2D finite element model was developed using
a cohesive mixed mode damage for the adhesive layer. The main objective of this work was to
determine the stress distribution along the bondline as a function of different parameters (patch
thickness, stacking sequence, overlap length…). One of the main findings of this study was the
influence of the overlap length on the failure stress of the repaired joint. For both single and
14
double lap joints, there is a critical value of the overlap length above which there is no strength
improvement.
Another study by the same authors [18] was interested in the mechanical behavior of single
and double-lap repair joints techniques. A parametric study was conducted on different
geometrical details (chamfering the patch outer face, thickening the adhesive near the overlap
outer edge, using fillets of different shapes and dimensions at the patch ends, chamfering the
outer and inner plate edges…). The effect of the shape geometry (single or double strap repair)
on the strength of the repaired structure and the stress distribution along the adhesive bondline
have been particularly considered. It was shown that with an optimal joint configuration, the
residual strength has been increased by 27% in the case of single-lap joints and by 12% for the
double-lap joints.
Later in [20, 21], Campilho et al. developed a two-dimensional (2D) finite element model for
internal scarf bonded repair joints. The aim of their work [19] was to propose a suitable finite
element model to simulate the tensile behavior of composites scarf repair structures. The main
conclusion was that the repair strength increases exponentially with the decrease of scarf angle.
Two different failure modes were observed for the repair. The first mode was observed for high
scarf angles (15°, 25° and 45°) and consists of an entire cohesive failure of the adhesive
bondline. The second failure mode was a mixed cohesive and interlaminar/intralaminar mode
failure which occurs for lower angles (3°). The difference in the failure mode was explained
by the authors as being related to the stress distribution variation along the bondline. In fact,
for higher angles, the bondline length is small and hence induces a higher stress distribution.
The model predictions in terms of failure load, relative displacement and initial stiffness were
15
also compared with experiments. A good agreement with experimental results was found on
these parameters.
Campilho et al. [20] continued the investigation of the mechanical behavior of flush scarf
repaired joints under tensile loading. As in [19], a two-dimensional (2D) finite element analysis
was performed using the cohesive mixed-mode damage model for the adhesive bondline.
Several scarf angles were studied. First, the shear and peel stress distribution along the adhesive
bondline was investigated. Then, a failure analysis was conducted to determine the strength
recovery of the repaired joint by varying the scarf angle and the laminate stacking sequence.
Peel stresses were less significant than shear stresses, for low scarf angles. Shear stresses had
peaks at the free edges of the bondline length, although these were less important than the ones
observed for lap joints [17-18]. This fact leads to an improvement of the strength of this type
of joints. The strength recovery of 2°- and 3°-scarf repaired specimens was about 100% for the
studied stacking sequences, except for the unidirectional lay-up ([032]), in which only a 47%
efficiency was obtained. However, for a 6°- scarf repaired specimen, the strength recovery was
seen to be dependent on the stacking sequence and a higher restitution was found for
[02/752/−752/902]2S stacking sequence reaching about 90% in comparison with 20% for a
unidirectional stacking sequence of [032]. With higher scarf angles (angles above 15°), a
reduction in the strength of the repaired joint was observed and the obtained efficiency was
below 40%.
Gunnion and Herszberg [21] carried out a parametric 2D finite element study of CFRP scarf
joints under tension loads. A linear elastic material stress analysis was performed. A local
coordinate system was defined to extract shear and peel stresses in the middle of the adhesive
16
bondline. Peel and shear peak stresses were evaluated for different combinations of
material/geometric parameters: scarf angle, adhesive thickness, ply thickness, laminate
thickness, over-laminate thickness and lay-up sequence. In particular, [90/0]2S, [0/90]2S, [45/0/-
45/90]S and [0]8 lay-ups were studied. The influence of laminate mismatch on peel and shear
stresses in the adhesive layer was also investigated. It was observed that the lay-up has a high
influence on the stress distributions, since stresses are higher near the 0º-plies. Using
unidirectional laminates, shear stresses are almost constant and peel peak stresses are observed
near the overlap edges. The influence of all parameters on peel and shear average and peak
stresses is summarized in Table 1-1.
Harman and Wang [14] performed a 2D elastic finite element (FE) analysis to validate the
developed analytical technique to optimize the shape of scarf joint between dissimilar
composites adherends. The developed FE model was used to evaluate the use of low stiffness
patch to repair CFRP composites structures. In this work, the authors investigated the influence
of the patch lay-up on the adhesive stress distribution. The optimized scarf repaired joint is
expected to enhance joint strength and to reduce the material to be removed. One of the main
conclusions of this work was that the variation of the scarf angle cannot minimize the shear
stress concentration in the adhesive bondline if the patch and parent laminates lay-up are not
identical.
A recent work from Bendemra et al. [22] has been conducted to study the tensile behavior of
both scarf and stepped flush bonded repair techniques in carbon-epoxy composite structures.
An elastic two-dimensional finite element model was developed. A parametric study was
performed in terms of parameters such as ply thickness, scarf angle, over-ply lap length and
17
lay-up, stacking sequence and adhesive thickness. Peel and shear stress peaks have shown a
strong sensitivity to the ply thickness, scarf angle and stacking sequence for both tapered scarf
and stepped repair joints. However, results showed that tapered scarf joints have a higher
sensitivity to adhesive thickness than stepped repair joints. For their material systems, a [-
45/90/+45/0]S laminate stacking sequence (i.e., parent structure and repair patch lay-up), an
adhesive thickness of 0.26 mm (increased from nominal thickness 0.13 mm), and over-plies
with a 5-mm lap length and [±45] stacking sequence were seen to be the optimal parameters
for a stepped joint repair. However, it should be noted that this set of parameters depends on
the ply thickness, the composite material, the adhesive film and the repair technique used.
Table 1-1 Parameters effects on the peel and shear stresses [21]
Parameter Average peel Peak peel Average
shear Peak shear
Lay-up No effect Increases if 0° plies
are in the outer
surfaces
No effect Decreases with more 0°
plies
Increases with increasing
distance between 0° plies
across the scarf
Laminate thickness No effect Decreases with
increasing laminate
thickness
No effect Decreases with increasing
laminate thickness
Mismatched
adherend
No effect Slight increase or
decrease depending
on lay-up
No effect Slight increase or decrease
depending on lay-up
Adhesive thickness No effect Increases with
increasing adhesive
thickness
No effect Increases with increasing
adhesive thickness
Scarf angle Increases with
increasing scarf
angle
Significant decrease
with scarf angle
increase
Decreases
with
increasing
scarf angle
Slightly decreases with
increasing scarf angles
Over-laminate Decreases with
increasing over-
laminate stiffness
Significant decrease
with increasing
over-laminate
stiffness
Decreases
with
increasing
over-laminate
stiffness
Significant decrease with
increasing over-laminate
stiffness
18
Three-Dimensional (3D) Analyses
Soutis and Hu [23–25] were among the first authors to study the behavior of composite scarf
repaired structures using a 3D finite element model. The studied structures were loaded in both
tensile and compressive loadings. With the developed model, the authors were able to
determine the stresses distribution in the adhesive bondline. Also, failure of the structure was
predicted and compared to experimental results. A main finding of this research was that the
optimal scarf angle was found to be 7° from the 3D model in comparison with an optimal angle
of 4° with the 2D model. This shows that a 2D finite element model gives conservative results
in comparison with a 3D model.
Pinto et al. [26] have developed a 3D finite element model to study the tensile behavior of scarf
repairs in carbon-epoxy structures using a ductile adhesive. The Cohesive Zone Model for the
simulation of damage initiation and growth in the adhesive layer was used. A parametric study
was performed on both the scarf angle and the laminate width to be repaired. It was found that
the strength increases exponentially with the reduction of the scarf angle. The addition of an
over-ply at the outer and bottom faces of the repair improves the strength recovery
approximately by 30 % and 60 %, depending on the scarf angle used.
Breitzman et al. [27] have studied the tensile behavior of scarf composite repaired joints using
a three-dimensional non-linear FE model. Only, the cohesive failure of the adhesive layer was
considered and the composite adherend failure was predicted using a static criterion applied to
the tensile fiber failure mode. The effect of the addition of an over-ply and its orientation was
examined and the scarf ratio was fixed to 1:20. It was observed that the addition of an over-ply
19
reduces the stress peaks at the junction of the 0°-plies. Another finding of this work was that
increasing the over-ply thickness has no major effect on the reduction of stress peak. A strength
recovery of 85% was obtained with one over-ply and an optimal quasi-isotropic stacking
sequence for the patch laminate.
Wang et al. [28] studied the mechanical behavior of stepped bonded joints under compressive
loading until failure. The authors developed a 3D FE model to determine the stress distribution
along the bondline and to predict the failure load and failure mechanisms of 3°-stepped joint
specimens. Geometrically linear and non-linear elastic analyses with failure criteria were
conducted. Hashin failure criteria and progressive damage laws were applied to the composite
laminates. Continuum shell elements were used for the FE mesh and cohesive elements were
placed between plies and on the interface between the adhesive layer and the composite
structure. Three configurations were studied: stepped joints with four and eight steps and a
scarf joint. The composites laminates had a [+45/02/-45/90]s stacking sequence. For the four-
step joints, each step contained two composite plies and for the eight-step joints, one step is
involved by ply. Experimental tests were also conducted for pristine composite plates, 3°-
stepped composite joints and impacted 3°-stepped composite joints. It was found that the
model predictions are in good agreement with the experimental results. However, for the
stepped joints, the finite element model considerably underestimates the compression-after-
impact strengths. The authors explained that this was due to the disbonding of the steps during
impact and concluded that further research was needed to resolve this under-prediction issue.
Also, they suggested that it is important to improve the design of stepped repairs to avoid
premature disbonding when the repaired structure is subjected to external impact.
20
Li et al. [29] developed a 3D finite element model to investigate the tensile performance of
CFRP scarf-lap joints. The model was based on cohesive zone elements for the adhesive
bondline and each ply of laminate was modeled by eight-node linear brick elements with
reduced integration (C3D8R). A thin layer of cohesive elements (0.01mm) was placed between
each 90°-ply and its adjacent layers. Three different stacking-sequences were used for the
composite adherends ([45/0/-45/90]s, [45/0/-45/90]2s and [45/0/-45/90]4s) and four scarf angles
were chosen (3.81°, 5.71°, 8.13° and 11.31°). The influence of these two design parameters on
the ultimate failure load, failure mode and lap shear strength were compared. The main
conclusions from this study are that the lap shear strength increases with the increase of the
scarf angle and that the failure load increases with the adherend thickness increase. It was found
also that the scarf joints have a stepped failure morphology in the adhesive bondline and the
major failure mode is a combination between cohesive failure and a delamination between the
90°-plies and its adjacent plies. Experimental tests were conducted and good correlations
between the test results and the numerical predictions were found in terms of failure load and
morphology.
Authors like Gunnion and Herszberg. [21], Bendemra et al. [22] have extended the 2D linear
elastic finite element models for rectangular patches to a complete 3D models for circular
patches. An identical shape for the peel and shear stresses was found using both techniques of
modelling in the applied stress direction. This result validates the use of 2D model for
parametric study.
21
1.1.4 Failure Mechanisms of Composite Bonded Joint Repairs:
Observations and Modeling Process
Experimental Failure Modes
The failure of composite bonded repair joint can be classified into different types of modes as
follow: adhesive, adherend, cohesive, or a combination of them. Figure 1-2 illustrates an
example of the adhesive, the cohesive and the mixed mode of failure of a bonded joint. To
study the failure morphology (or mode) and the load carrying capacity of repaired composite
structures, two types of repaired joints are usually manufactured: rectangular (2D) joints and
circular (3D) joints. For the first type, called 2D or rectangular joint, the repair is across the
whole width of the specimen and it is relatively simple to manufacture. This joint is widely
used in the literature and provides useful information about the failure mechanics of the
repaired joint. It can be easily modeled by a 2D finite element model assuming a plane strain
problem. Generally, specimens with 2D joints were loaded under tension [16, 20, 30–32], as
can be seen in Figure 1-3. The second type, called circular or 3D joints (because a two-
dimensional cross-section assumption can no longer be made), is more complex to
manufacture. This type of repair is representative of a true repair that could be applied in a
damaged structure. These repaired joints are tested under tension, compression or bending
loads in the literature.
22
Figure 1-2 Failure mechanisms of a bonded joint
Figure 1-3 A tension-loaded 2D scarf joint used in the literature [31]
One of the reports published by the US Air Force [32] was interested in the failure mechanics
of a 2D scarf composite joint under tensile loading, at room temperature conditions. The
authors have used an electron microscope to analyze the failure surface of the tested specimens.
The specimens were carbon-epoxy composite plates with a quasi-isotropic stacking sequence
[02/±45/90/±45/02]s. The main observations made in this report were that:
For low scarf angles (1.1°, 1.9° and 3°), the failure mode was complex. As shown in Figure
1-4, failure begins at one of the free scarf joint ends and continues through the adhesive. At
23
point B, many 90° and 45° plies fibers were pulled out. Then, failure was forced in the
adhesive surface with the presence of the 0° plies. Then failure extended to point C and a
considerable amount of delamination was observed (point C to point D).
For high scarf angles (6.2°, 9.2°), the failure occured mainly in the adhesive bondline.
Specimens contained also some regions where failure occured in the composite adherend.
Charalambides et al. [16] reported the efficiency of 2°-scarf joint specimens with overlapping
plies under static tensile loading for dry, four-months and 16-months conditioned specimens.
Temperature and moisture were found to affect the scarf joint failure mechanisms considerably.
It was shown that for the dry specimens, failure occurred in the parent side of the joint and
seemed to originate from the end of the longest overlap plies (‘Type A’), as illustrated in Figure
1-5. All the four-month conditioned joints showed a failure of ‘Type B’ and the 16-month
conditioned specimens showed ‘Type A’, ‘Type B’ and ‘Type D’ failure modes originating
from the end of the shortest overlap plies. The authors [16] explained that the failure of ‘Type
A’ is caused by the presence of high through-thickness stresses at the end of the overlap plies
which led to the formation of delamination and then caused a final catastrophic failure when a
critical value of the applied load was reached. Failure of ‘Type B’ seemed to be caused by high
longitudinal stresses. For the four-month specimens, no cracks or delamination under the long
overply plies were observed. The change in the failure path and the small increase in the static
failure load, implies that conditioning for four months might have caused an increase in the
through-thickness strength of the composite.
A circular patch repair was tested under tensile loads by Xiaoquan et al. [30]. It was observed
that the specimens failed through the middle of the scarf repaired region and the patch remained
24
attached to one-half of the plate, as seen in Figure 1-6. They observed also that fracture in the
top surface was neat and smooth in comparison with the bottom one. Electron microscopy was
used to have more details about the fracture of the specimens. It was observed that microcracks
are initiated through the weakest part of the interface. These microcracks lead to the formation
of a main crack, which spreads rapidly through the adhesive bondline when a critical value of
the load is reached.
Figure 1-4 Failure morphology of a low scarf repair joint angle under tensile load [31]
Figure 1-5 Failure paths observed in the static tensile 2°-scarf repaired joints under
different environmental conditions [16]
25
Figure 1-6 Failure morphology of a circular patch repair: (a) top surface (b) bottom
surface (adapted from [30])
Numerical Modelling of the Adhesive Joints
i. Cohesive Zone Element Technique
Several research work has been conducted to predict damage in adhesively-bonded composite
structures. Most of them [17, 20, 26, 29-30] use cohesive element models (CZM), with
triangular law, to simulate the adhesive layer damage. The CZM, with triangular law, simulates
damage by the application in most cases of a bi-linear traction-separation law between initially
coincident nodes (see Figure 1-7. a), which assumes first a linear elastic behavior of the
adhesive followed by a linear evolution of damage in the softening phase.
Researchers [34, 35] used also trapezoidal laws to simulate the behavior of adhesively-bonded
joints. For trapezoidal laws, the adhesive stiffness in opening or shear modes is the initial
stiffness of the adhesive for each pure mode. Then a plateau region is introduced to represent
the ductile behavior of the adhesive (see Figure 1-7. b) that is followed by a linear softening
with increasing damage until failure.
26
The cohesive zone element model (CZM) has the advantage of being able to model the behavior
of joint surface from its linear behavior, to the initiation and propagation of damage up to the
final failure in a single analysis.
Another advantage of CZM is the ability to predict the occurrence and propagation of an
interfacial crack without prior knowledge of the location of the initiating microcracks. These
models introduce cohesive elements of zero thickness at the joint plane between two substrates
of any material (which is a limitation of CZM models since one must know a priori where to
place CZM elements in the FE mesh).
For a traction-separation law, the stiffness matrix relating the traction stresses and
corresponding separations in tension and shear across the interface is defined by:
0 0
0 0
0 0
n nn n
s ss s
t tt t
K
K
K
(1)
where: n s t are the relative displacements in normal and transverse shear directions and
[K] is the stiffness matrix whose components can be defined as EKnn ta
and ss tt
a
GK K
t
where E is the adhesive elastic modulus, G is the shear modulus and ta is the thickness of the
adhesive.
27
ii. Elastic-Plastic Models for the Adhesive
As adhesives can reveal a non-linear behavior, plasticity models can be used to predict their
mechanical behavior and their failure mechanisms adequately. In the literature, different
plasticity models have been used [35, 37]. The Drucker-Prager plasticity model [36, 38] is well
suited for describing a pressure dependent hardening material such as epoxy adhesives and
gives results that reproduce accurately the experimental strain hardening data [36, 38].
However, this model requires much more material parameters [37] for plasticity than a classical
metal plasticity model based on the von Mises criterion that is often used because of its
simplicity.
Figure 1-7 Cohesive zone models’ presentation: (a) triangular law, (b) trapezoidal law
[20].
a. Von Mises Yield Criteria
Many authors [37, 38, 40] used the von Mises criteria to represent the mechanical behavior of
the adhesive. This criterion is a simple yield criterion that expresses yielding as a purely shear
deformation process which occurs when the effective shear stress reaches a critical value
[37, 38]. The plastic properties of the adhesive can be determined from a ASTM D5656 Thick
a) b)
28
Adherend Shear Test (TAST) [39]. During the test, the adhesive is supposed to be subjected to
pure shear stress.
b. Drucker-Prager Yield Criteria
Most adhesives under shear and compression stresses show a sensitivity to the hydrostatic
pressure especially for polymeric/toughened adhesives [37]. As the von Mises criterion cannot
take into account these hydrostatic stresses, a more complete criterion based on a simple
modification of the von Mises criteria, named the Drucker-Prager (DP) model [36, 38], includes
this sensitivity, and the simplest one is a linear DP yield criterion, given by
0e m (2)
where 0 is a material parameter related to the shear yield stress τs by:
0 3 s (3)
and m is the hydrostatic stress given in terms of principal stresses (σ1, σ2, σ3) by:
1 2 3
1( )
3m (4)
So from equations (2) to (4), it can be observed that the parameter μ is dependent on the
adhesive material and characterizes the sensitivity of yielding to the hydrostatic stress [35].
This parameter can be determined from shear and tensile tests using:
3 [ 3 1]s
T
(5)
where T is the stress from the tensile test.
29
In this work, the discussed failure mechanism is limited to answering the following question:
which part or section of the structure reach failure first and the failed part is expressed by a
failure model (dynamic failure supported by ABAQUS. Hence further aspects such as initial
and final crack length, crack growth /propagation or energy release rate are not of interest here.)
1.1.5 Review Summary
The above review covered various aspects of design, finite element simulations and failure
mechanisms of bonded joint repairs of monolithic composite structures. Table 1-2 summarizes
the different issues and aspects studied in the literature and reviewed in this chapter.
Table 1-2 Issues and aspects studied in the literature for composite bonded repairs
Joint geometry
Composite
Material
Finite element
models
Simulation of the
adhesive layer
Cure of the
repair patch Cure method
Single/double lap
Scarf-scarf
Step-step
Unidirectional
(UD)
2D
3D
CZM
Elastic-plastic
Pre-cure
Co-cure
Autoclave
Oven
1.2 A Review of Honeycomb Sandwich Panel Bonded Repairs
After reviewing the monolithic composites bonded repair technology in section 1.1, a literature
review of honeycomb sandwich panel bonded repairs techniques is presented in this section.
Sandwich panels are being used in many industries such as aerospace, and automotive for
different applications. One of the main interests of sandwich structures is their high specific
flexural rigidity. They also offer many advantages: lightness, mechanical strength, reduced
maintenance, complex shapes. Sandwich structures have gained popularity in the aeronautical
30
field. On the Airbus A380 aircraft, for example, sandwich structures are used in nacelles,
ailerons, floor, fuselage, cabin, etc. However, despite their good properties, honeycomb
sandwich structures are sensitive to impact damage, which can cause disbonding, delamination
and internal crushing. Considering their extended service life and operating conditions, the
extent of damage determines whether the sandwich components need to be repaired or replaced.
Hence, to take full advantage of their many benefits, the improvement of their performance
requires one to ensure first that these structures are durable, repairable, and maintainable. Since
fiber-reinforced composite sandwich structures are increasingly being used in primary aircraft
components, it has become necessary to develop effective repair methods that will restore the
component’s original design strength without compromising its structural integrity.
This section begins with an introduction on sandwich panels presenting their components,
benefits and drawbacks. Different failure modes for sandwich panels will be discussed as well.
Then, a detailed review of the literature on honeycomb sandwich panel repairs will be
presented. Here, the focus is on both the experimental studies and the numerical methods
developed to study the mechanical behavior of repaired sandwich panels under different loads.
Finally, a conclusion and the main settled or still open issues of the literature will be presented.
1.2.1 Introduction
Typically, sandwich panels are composed of two thin skins (or facesheets) made either from
metallic materials or from fiber-reinforced composite materials, and a thicker core material,
generally an aluminum or a Nomex honeycomb material in between as shown in Figure 1-8.
The figure indicates the nomenclature used to define the different geometric characteristics of
31
the sandwich panel. Core materials, generally low-density material, are usually in forms of
honeycomb or foam structures. Metallic (aluminum) or polymeric materials are the most
common materials used for the core. The concept behind sandwich structure is that the skins
carry the in-plane compressive and tensile stresses resulting from the applied bending moment,
while the main function of the light-weight core is to keep the two skins apart and to resist and
transfer the shear forces to the skins. By increasing the thickness of the core, the flexural
rigidity of the panel increases for a small weight penalty [40].
Table 1-3 shows the flexural stiffness and strength advantages of sandwich panels in
comparison with solid panels.
Figure 1-8 Nomenclature used to describe the sandwich panel geometric characteristics
Table 1-3 Structural efficiency of sandwich panels in terms of weight [41]
32
Relative bending
stiffness 1 7 37
Relative bending
strength 1 3.5 9.2
Relative weight 1 1.03 1.06
During service, sandwich panels are subjected to various stresses which can cause damage, the
accumulation of which can lead to their rupture. Sandwich structures remain also vulnerable to
impact damage including damage resulting from maintenance activities such as dropped tools.
Therefore, it is important to understand the main modes of deformation and damage, which can
result from the various loads to which they may be subjected in service conditions.
Honeycomb sandwich structures can fail in several ways. Depending on the geometry of the
sandwich panel and the loading type, different failure modes can be induced and set limits on
the mechanical performance of the sandwich structures. Failure of the sandwich structures may
be driven by the strength of the facesheet, core, or adhesive, by a local instability mode such
as facesheet wrinkling or facesheet dimpling, or by general instability such as global buckling
[42]. The failure load and the corresponding failure mode depend strongly on the properties of
facesheet, core and adhesive materials. The typical observed failure modes are presented in
Figure 1-9 and briefly described as follow.
Facesheet Failure
Different failure modes can occur in the skin of the sandwich panel: face wrinkling, skin
yielding and intra-cell dimpling.
i. Facesheet Yielding
33
In this case, failure occurs when one or both facesheets fails by yielding or fracture, as
presented in Figure 1-9.a. The criterion for failure is that the stress in the facesheet material,
𝜎𝑓𝑐𝑟 , exceeds its allowable stress, Y .
𝜎𝑓𝑐𝑟 ≥ 𝜎𝑌 (6)
ii. Facesheet Wrinkling
This is a type of local instability characterized by buckling of the facesheet. The buckling may
occur either inwards or outwards the core, depending on the stiffness of the core in compression
and on the adhesive strength, as presented in Figure 1-9.b. This failure is most prevalent with
thin facesheets and low-density core. The critical compressive stress that results in wrinkling
is given by Allen [42], as
𝜎𝑓𝑐𝑟 = (3/(12(3 − 𝜈𝑐𝑥𝑧)2(1 + 𝜈𝑐𝑥𝑧)2)−1/3) 𝐸𝑓𝑥
1/3𝐸𝑐3
2/3 (7)
where νcxz is the out-of-plane Poisson ratio of the core and Ec3 is the out-of-plane elastic
modulus of the core.
iii. Facesheet Dimpling
Facesheet dimpling is also known as intra-cell buckling. It is a type of local instability
characterized by local buckling of a facesheet induced from the non-continuous facesheet
support by the core. This failure mode occurs when the facesheets are thin and the cell size is
large, as seen in Figure 1-9.c.
34
Core Failure
i. Core Shear Failure
The core shear failure occurs when the applied shear stress exceeds the transverse shear
strength of the honeycomb core. This usually results in cracks inclined at 45° to the midplane.
The core material is mainly subjected to shear since it carries almost the entire transverse load,
and very little in-plane load. Low density honeycomb cores are very sensitive to this failure
mode. The transverse shear strength is given by [43]:
𝜏𝑐𝑟𝑠ℎ𝑒𝑎𝑟 = 𝜏𝑐𝑥𝑧 =
𝑡𝑐𝐺𝑐𝑥𝑧
2𝑡𝑓 (8)
where Gcxz is the core transverse shear modulus, tc and tf are the thickness of the core and
facesheets respectively, as illustrated in Figure 1-9.d.
ii. Core Crushing
This failure mode occurs when the facesheets move towards each other under the influence of
bending or through-thickness loads. This mode occurs when the core material has insufficient
compressive strength, as presented in Figure 1-9.e.
Global Buckling
The global or general buckling of a sandwich panel is a general instability of the structure, and
is similar to the classical buckling of plates or columns. Both facesheets and core remain intact
in this type of failure, as seen in Figure 1-9.f.
35
Figure 1-9 Different failure modes of a sandwich panel [43].
1.2.2 State-of-The-Art Review of Sandwich Panel Repairs
Typical Repair Procedure for Sandwich Panels
As for the monolithic composite laminates, different repair configurations exist for sandwich
honeycomb panels. Two types of bonded repairs can be used to repair a honeycomb sandwich
panel: an external type of patch repair and a scarf-type of patch repair.
The typical scarf-type repair procedure of honeycomb sandwich panels involves the removal
of the damaged area of the skins with or without core removal. The edges of the parent plies
are scarfed or stepped. The surface is cleaned and prepared to receive the adhesive and repair
plies. The damaged region is then repaired by inserting a core plug if it is necessary and
stacking skin plies with a similar or non-similar lay-up as the parent ones. These new parts are
36
bonded to the parent structure using an adhesive film. The scarf-type repair procedure is
illustrated in Figure 1-10.
Figure 1-10 Typical scarf-type repair procedure of a honeycomb composite sandwich panel
Experimental Characterization of the Honeycomb Sandwich Repair
Unlike monolithic composite structures, works on repair of sandwich panels are quite few and
limited. Different studies [44–47] have been carried out on repair techniques and
characterization of repairs on sandwich structures. Different repair techniques and processes
have been discussed in some works. The use of high and low temperatures cure cycles has been
discussed several times as in [44, 48]. It has been demonstrated that repairs cured at high
temperature show a better restoration of the strength.
The AGARD (Advisory Group for Aerospace Research & Development) [44] published a
report on repairs of sandwich structures used in military structures. Here, three different
techniques are used to repair the sandwich structure with an external patch. The patches were
37
either co-cured or pre-cured and the core either replaced or filled with a filler paste cured at
high and low temperatures cycles. Static and fatigue compression tests were carried out to
characterize the quality of the repairs. Results showed that the pre-cured patch method is the
most suitable for field-level application.
Baker et al. [45] have studied experimentally a scarf repair on a horizontal stabilizer of a F/A-
18 spacecraft composed by an Aluminum honeycomb core and CFRP skins. The repaired
structure was tested under a four-point bending load. The specimens were tested at -40ºC, room
temperature and 104ºC, in dry and wet conditions. The failure of the adhesive film was cohesive
for all test conditions. At 104ºC, the failure strains were reduced by 50%, compared to the
specimens tested at room temperature.
Rider [46] conducted a study on in-situ repairs of sandwich structures of an F-111 aircraft.
Several problems were noted during this study concerning the repair technique used. Among
the critical points studied are the humidity in the core and the importance of having an adequate
drying step for the core to avoid problems of detachment of the patch. An alternative was
proposed: after a drying step of two hours at 100 °C, surface preparation is performed followed
by a storage of the structure at 50°C which is advised before proceeding with the repair.
In the literature, rectangular and circular repair patches on sandwich structures (see Figure
1-11) were subjected to different loadings (four-point bending, tension, shear, and
compression) to determine their mechanical strength. Rectangular or 2D repair configurations
were studied under different loading in [2, 47]. Circular repairs were tested, at ambient
temperature, under edgewise compressive loading in [49, 50].
38
Figure 1-11 Scarf-type repair patches on honeycomb sandwich panel
Mahdi et al. [47] tested rectangular sandwich panel repairs (2D configuration) under four-point
bending load. Here, the scarf repair has a plain weave overply ply with a (+45/-45) lay-up and
results are obtained for a non-symmetric sandwich structure (the repaired skin lay-up is [(+45/-
45)/ (0/90)] and the undamaged skin lay-up is [(0/90)/ (0/90)]). The repaired facesheets were
loaded in both compression and tension. Two repair configurations were studied: overlap and
scarf repair. The repair was cured at low and high temperature systems. The main findings of
this work are that when loaded in compression, the scarf repairs were weaker than overlap
repairs. However, scarf repairs were stronger in tension achieving 100% of the pristine strength.
Finally, the cure temperature had no major effect on the strength recovery of the repaired
sandwich structures.
A series of experimental tests (tensile, shear and four-point bend tests) were conducted by
Tomblin et al.[2, 51] to study the effects of different process parameters on the quality of 2D
sandwich panel repairs. The repair carried out included a core removal and replacement. Two
39
different cell sizes for the core plug were considered in this work [2]: 3.175 mm and 9.525 mm.
Most of the repaired specimens tested under different loads showed a high recovery of the
residual strength (about 92%). It has also been proven that the size of the core cell plays an
important role on the performance of the repaired sandwich structure. The core with a 3.175
mm cell showed better strength recovery than one with a 9.525 mm cell size. A damage
tolerance analysis on sandwich structures was included as well [51]. As a conclusion of their
work, a methodology for the repair process along with design tools for damage tolerance on
sandwich structures were developed.
Like for composite bonded joint repairs, the scarf angle is an important parameter to consider
in the design of repairs in sandwich structures [45, 47, 52]. Several scarf angles (3°, 6°, and 9°)
[52, 53] or ratios (1/10, 1/20, 1/30 ...) [45, 54] have been studied. The results of these studies
show that with a smaller angle, a better restoration of the strength is found.
Fatigue resistance of repaired sandwich structures has also been studied in [44, 55]. But the
work in this area is very scarce. The AGARD group [44] published fatigue results on sandwich
structures loaded in compression. It showed that the repair with high temperature cure cycle
has a higher recovery than the one with low cure temperature.
Mahdi et al. [48] performed cyclic four-point bending fatigue tests on pristine (undamaged)
and 2D repaired sandwich beams. Three configurations, as for the static work [47], were
studied: an overlap and two scarf repairs. All configurations were tested in tension and in
compression. Also, two cure cycle systems were used like in [47]. From this study, the authors
showed that the overlap repair performed better in compression than the scarf repair
40
configuration. The degradation of stiffness with cycling was also investigated and was related
to the microscopic evolution of damage.
Finite Element Analyses of Honeycomb Sandwich Panel Repairs
Numerical models, with different levels of complexity, have been developed to predict the
mechanical behavior of repairs in sandwich structures. 2D elastic models, based on the
assumption of plane strain formulation, with a linear elastic behavior of the adhesive joint have
been developed in the majority of studies ([52, 53]). The purpose of these models is to
determine the distribution of shear and peel stresses along the adhesive bondline. The
distribution of stresses in scarf and overlap types of repairs was compared [52]. It has been
demonstrated that scarf repair has a homogeneous stress distribution in comparison to the
overlap repair. The peak stresses are greater at the overlap level than everywhere else. Later,
3D finite element analysis with a progressive damage model for the composite skins were
performed to study the mechanical behavior of the repaired sandwich structures under
compressive loads [49, 50].
i. 2D Finite Element Analysis
Oztelcan et al. [53] presented a finite element study on repaired sandwich helicopter blades
with GFRP facesheets and honeycomb core under a compressive loading. In this work, two
repair configurations were evaluated: an overlap repair and a scarf repair. The numerical
models used eight-node reduced integration shell elements (S8R) for the composite skins,
available in Abaqus [56]. First, a global model was used to identify the most stressed regions
of the structure, and then a smaller local model was built for the critical region and only for the
41
composite facesheets. This local model was subjected to the displacements obtained from the
global model. A subroutine was developed for the adhesive layer elements, including a
progressive damage model based on the Maximum Stress Criterion to obtain the shear stress
distributions in the adhesive. For the overlap configuration, shear stress distributions presented
a parabolic shape, symmetric relatively to the overlap central region, and peaking at the overlap
edges. The scarf repair used an angle of 3º and the parent and patch had the same lay-up. A
uniform shear stress distribution was obtained in comparison with the overlap configuration.
Moreover, increasing the compressive load, the adhesive layer was kept uniformly loaded along
all its length, resulting in a more efficient distribution of stresses, compared to the overlap
repairs.
Mahdi et al. [54] used 2D finite element models to predict the performance of both pristine and
scarf repaired sandwich panels subjected to static and fatigue four-point bend loading.
Numerical analysis results showed a good correlation in terms of stiffness prediction of both
undamaged and repaired coupons. An attempt to calculate the failure strength of the studied
sandwich beams has also been made. The Tsai–Hill criterion was chosen to predict the first-
ply failure load. However, the failure load prediction was problematic and did not show a good
correlation with experiments.
Another 2D model using cohesive elements was also developed by Chen [57]. The model was
used to study the behavior of adhesively bonded 3°-scarf-repaired sandwich structure under
four-point bending load. Good correlation between the experimental results and the numerical
predictions was found in terms of the failure load, the residual stiffness and the crack path.
42
Ramantani et al. [52] investigated the mechanical performance of repaired honeycomb panels
by numerical models using interface elements, in order to obtain the distribution of stresses at
the critical points in the adhesive joint. A 2D symmetric finite element model with a mixed
cohesive approach was developed to simulate the behavior of the repaired structure under a
four-point bending load. Scarf and overlap repair configurations were studied. The influence
of the scarf angle variation (3°, 6°, 9° and 15°) for the scarf repair and of the thickness of the
repair (thin/thick) for overlap repairs were investigated in terms of the restoration of residual
strength and stress analysis. The scarf repair with an angle of 3° showed a better distribution
of shear stresses. This was due to the fact that the adhesive joint is longer with a 3°-scarf angle.
The failure mode was also dependent on the scarf angle variation. For overlap repairs, it was
also proven that the ultimate failure load is strongly influenced by the overlap length and that
from a critical length of the overlap, there will be no influence on the ultimate load.
ii. 3D Finite Element Analysis
Baker [45] has developed a 3D finite element model to study the stresses distribution along the
adhesive bondline of a typical repair of a graphite/epoxy honeycomb sandwich structure. A
scarf angle of 3° was chosen for the repair configuration. Predictions of the shear stress
distribution along the adhesive joint have been compared with experimental results. The main
finding of this work is that the shear stress along the bondline is not uniform as is the case of
isotropic adherend.
Mahdi et al. [54] used a quasi-3D finite element model to predict the performance of both
pristine and scarf repaired sandwich panels subjected to static four-point bend loading.
43
Numerical analysis results showed a good correlation with the developed 2D model and the
experiment in terms of stiffness prediction of both undamaged and repaired coupons. However,
the ultimate load was problematic and did not show a good correlation with experiments.
The compressive behavior of circular repaired sandwich panels was investigated by Liu et al.
[49]. Both experiments and finite element analyses were conducted to study the influence of
repair variables such as scarf angle and cure cycle on the quality of the repair. A progressive
damage model, based on the Hashin’s criterion for unidirectional composite materials, was
developed and used to predict failure of the repaired sandwich panel. The adhesive film was
modeled using cohesive elements. Good correlation between experimental and numerical
results was obtained. However, since the inner diameter of the repair was small (25mm)
compared to the sandwich panel width (100 mm), the load is by-passed, and failure occurs in
the parent and not in the adhesive bondline
A recent study from Zhang et al. [50] was conducted to investigate the mechanical performance
of pristine, open-hole damage and circular scarf repair honeycomb sandwich panels under
compressive loads. A 3D finite element model was also developed. A failure criterion based
on the Hashin’s criterion with a progressive damage evolution was included for the quasi-
isotropic composite skins. The adhesive layer was modelled using cohesive elements. The
honeycomb core cells were modelled using shell elements. The honeycomb material was
considered as an elastic-plastic material. A good agreement was found in terms of ultimate
failure load and damage shape between the experimental and numerical results. Failure of the
repaired sandwich panel was due to adhesive delamination and local buckling of the patch.
Although the developed model is accurate, the computing time was quite long. Another finding
44
of this work was that the structure strength increases with the decrease of scarf angle and that
the optimum number of 0°-overplies was one to reach the highest strength.
1.2.3 Concluding Remarks
This review highlights the state-of-the -art on different topics that will be developed further in
this thesis. It allows a clear assessment of the contribution of this research. According to the
preceding literature review carried out on the repairs of sandwich structures, important issues
that retained our attention can be summarized as follows:
i. From the Experimental Point of View:
Most repairs were performed on unidirectional composites. Repairs on woven
composites have been very scarcely studied in the literature [2, 47].
The scarf-scarf type of joint was chosen as the repair configuration in most
cases. This implies that the repair patch needs to be pre-cured.
The curing of the parent structure as well as of the repair patch was done under
autoclave in most cases.
The characterization of the repair was often carried out at ambient temperature
conditions and the influence of other temperature conditions was barely studied.
Table 1-4 to Table 1-6 regroup the different experimental aspects studied in the literature on
sandwich honeycomb repairs.
45
ii. From a Numerical Point of View:
Linear elastic 2D finite element models have been developed to study the distribution of
stresses in the adhesive joint.
Cohesive elements were chosen to predict the rupture of the adhesive joint. This type
of element cannot, however, be used for the modeling of stepped-scarf repair joints.
A single study [52] was carried out on the effect of different parameters (angle.) on the
behavior of sandwich panel repairs. This study was carried out using a 2D finite element
model using cohesive elements for scarf-scarf repairs.
3D models were developed to predict the mechanical behavior of sandwich panel with
circular repairs until rupture. Failure criteria for unidirectional composite material were
used.
Table 1-7 summarizes the different aspects of the finite element models studied in the literature
for the sandwich honeycomb panel repairs.
Table 1-4 Sandwich panels component materials used in the literature
Skin Materials Honeycomb core Adhesive film
Baker [45] AS4/3501-6 U.D prepreg Aluminum alloy core FM300K
Tomblin [2] Prepreg and wet lay-up material Nomex honeycomb core FM377S
Mahdi [47] F914C woven fabric Nomex honeycomb core Redux 319A
Ramantani [52] CFRP U.D prepreg PVC foam core Epoxy resin
Liu [49] MTM44-1/HTS(12K) U.D
prepreg Nomex honeycomb core FM490A
Zhang [50] CFRP U.D prepreg Nomex honeycomb core
46
Table 1-5 Repair configuration, process and cure methods for sandwich panel repairs
used in the literature
Repair configuration Cure temperature Cure method
Tomblin [2] Scarf-step Low & high
temperature -
Mahdi [47] Scarf-step Low & high
temperature Oven/ hot bonder
Liu [49] Scraf-scraf Low & high
temperature Autoclave
Zhang [50] Scarf-scarf - Autoclave
Table 1-6 Mechanical characterization and non-destructive inspection of sandwich panel
repairs used in the literature
Test loading Environmental
conditions
Non-destructive
inspection
Tomblin [2] Four-point bending, tension, shear Room temperature C-scan, Tap Test
Mahdi [48] Four-point bending Room temperature -
Liu [49] Compression Room temperature -
Zhang [50] Compression Room temperature C-scan
Table 1-7 Finite element model types used in the literature for sandwich honeycomb
panels
Finite element
analysis Behavior of the adhesive Behavior of the composite skins
Ramantani [52] 2D Cohesive elements -
Mahdi [54] 2D, quasi-3D - Failure of first ply-Tsai-Hill criterion
Liu [49] 3D Cohesive elements Progressive failure damage- Hashin criterion
Zhang [50] 3D Cohesive elements Progressive failure damage- Hashin criterion
47
Chapter 2.
Overview of the Problem and Research Focus
2.1 Rationale of the Thesis
The main goal of this study consists in designing a reliable bonded repairs methodology for
primary sandwich honeycomb structures for aerospace applications, and particularly in
developing simulation tools and protocols for the design of sandwich composite bonded
repairs. For that purpose, a series of experimental investigations and numerical simulations of
repaired bonded honeycomb sandwich panels will be conducted.
In that regard, a state of the art literature review was performed and revealed the following
issues:
The composite materials used for the repair of sandwich panels are in most cases
standard unidirectional carbon-epoxy prepreg cured in an autoclave and the stacking
sequence for the parent and the repair patch uses only 0o or 90o plies.
Parent structures and repairs made with woven fabric composite have been very
scarcely studied in the literature. However, these materials are now widely used to
manufacture primary aerospace structures.
In most cases, repairs are cured in autoclave. However, in practice, repairs are processed
either using a hot-bonder or a heat blanket.
48
Image correlation systems to evaluate the strains on the repair patch have been scarcely
used. The use of such technique is however very helpful to observe the strain
distribution on the repair patch and understand how failure occurs.
Finite element models developed to study the mechanical behavior of repaired
sandwich panels use cohesive elements to discretize the adhesive joint. However,
cohesive elements cannot describe adequately the elastic plastic behavior of the
adhesive and relies on parameters which are difficult to evaluate.
The use of progressive damage models for unidirectional composite materials to predict
failure of the composite patch is very limited in the literature. The application of
progressive damage model to predict failure of patches made with woven-fabric
material has, to our best knowledge, never been discussed in the literature.
Finite element analyses have been so far conducted either on scarf-scarf or stepped-
stepped repair joints. In practice, stepped-scarf repair joints are widely used. This type
of repair has been simplified to a scarf-scarf configuration in finite element analyses
presented in the literature. This simplification may lead to inaccurate stress predictions
in the adhesive joint.
In most cases, the developed finite element models are not validated with experimental
results.
Based on the project main objectives and the summary of the literature review, sub-objectives
have been defined and will form the core of this thesis. They are described in the next sub-
sections.
49
2.1.1 Assessment of the Mechanical Behavior of Honeycomb Sandwich
Panels with Bonded Repairs by Experimental Testing
The first objective of this thesis focuses on the determination of the mechanical performance
of repaired honeycomb sandwich panels under different static loadings: tension, compression
and four-point bending. Two repair configurations will be used for this experimental program
(Figure 2-1):
2D repair where the repair patch has a rectangular shape and is across the whole specimen
width.
3D repair where the repair patch has a circular shape (which is widely used in practice).
Figure 2-1 Repair configurations in sandwich honeycomb panels
50
2.1.2 Development of Finite Element Models for Better Understanding and
Accurate Prediction of the Mechanical Behavior and Failure Modes of
the Repaired Sandwich Panels under Different Loadings
The second objective consists in the development of finite element models to be used as an
alternative design tools for sandwich panel repairs. Different models will be developed to
predict the mechanical behavior of the repaired sandwich panels until failure for different
loadings. These models will take into account an elastic-plastic behavior of the adhesive based
on physical parameters in comparison with the cohesive element models proposed in the
literature.
2.1.3 Validation of the Finite Element Models and Conduction of a
Parametric Study
The proposed models will be validated with experimental results. Once validated, these models
will be used to perform a parametric study to investigate the effect of different design
parameters on the strength recovery of the 2D repaired sandwich panels under tensile loads.
The results of this parametric study will be used as a guideline to select appropriate design
parameters for a given repair configuration of a honeycomb sandwich structure. The design
parameters are:
The scarf angle
The thickness of the sandwich skin
The use of an overply and its overlap length
51
2.2 Methodology and Thesis Structure
2.2.1 Methodology
Figure 2-2 outlines the methodology followed to reach the research objectives.
Figure 2-2 Flowchart of the research methodology
Experimental tests
The experimental work is divided into two main parts:
Part I: Mechanical Characterization of the Sandwich Honeycomb Constituents
Here, the mechanical properties of the constituent materials of the sandwich panels, namely the
CFRP facesheets and the honeycomb core, will be evaluated. This task will be achieved by
conducting static tensile and compressive tests, according to ASTM standards. The determined
mechanical properties of these components will be implemented later in the developed finite
element models. This is discussed in chapter 3.
Characterization tests:
- Composite skins
- Nomex core
- Adhesive film
FE models of the repaired
sandwich composite panels
Compressive, tensile and four-
point bend tests on repaired
sandwich panels Model validation
Experimental tests Numerical simulation
52
Part II: Mechanical Performance of the Repaired Sandwich Panels
Experiments will be conducted on pristine and repaired sandwich panels (2D and 3D repair
configurations) to investigate their mechanical behavior under different loading (tension,
compression and flexure). Tensile, compressive and flexure strength of the repaired specimens
will be compared with the pristine values. This is discussed in chapters 4, 5 and 6.
Finite element modelling
Two-Dimensional Finite Element Model (2D FE Model)
First a two-dimensional (2D) finite element model will be performed using the software
package Abaqus [58]. The main objectives of this FE model are to study the stresses
distribution along the adhesive bondline and to predict the mechanical behavior of the 2D repair
until failure. The corresponding model geometry is easy to create. Since the repair will be
across the width, it can be represented by a longitudinal-longitudinal-cross section (see Figure
2-3) so that plane strain assumptions can be adopted for the analysis.
As a start-up, a 2D linear elastic analysis will be conducted to determine the peel and shear
stresses distribution along the adhesive bondline. Next, a second analysis will be undertaken
and will take into account the nonlinear behavior of the adhesive film, to predict the mechanical
behavior up to failure of the 2D repair under tension and four-point bending loads. This will be
discussed in chapters 3, 4 and 5.
Three-Dimensional Finite Element Models (3D FE Model)
The second finite element model to be developed is a three-dimensional (3D) model which
takes into account the progressive damage of the woven-fabric facesheets and the elastic-plastic
53
behavior of the adhesive film. Because of the symmetry of the problem, a quarter of the model
geometry will be modeled, as presented in Figure 2-4. This model will allow predicting the
compressive mechanical behavior of pristine, open-hole damage, and circular repaired panels.
The finite element model predictions will be experimentally validated. This is discussed in
chapters 6 and 7.
Figure 2-3 Longitudinal-cross section modeled with 2D model
Figure 2-4 Circular 3D model geometry
Adhesive
Bag face
Nomex core Patch
Parent
54
The experimental and numerical investigations performed in the thesis used mainly the
following material system and processes:
Two out-of-autoclave woven-fabric prepreg materials: the plain weave (PW) and the
eight-harness satin (8HS),
A four-ply sandwich panel skin with a quasi-isotropic sequence,
A realistic repair geometry, which is a flush stepped-scarf repair geometry (for both 2D
and 3D repair configurations),
Out-of-autoclave and co-bonded repair patch.
2.2.2 Chapters Presentation
The thesis is then organized as follow.
Chapter 3 presents the experimental work done to determine the mechanical properties of the
sandwich panel constituents, namely the facesheets and the core. First, a series of tensile and
compressive tests is performed to determine the in-plane and out-of-plane mechanical
properties of the constituents. After that, the developed 2D and 3D finite element models are
verified, and numerical predictions of the laminate behavior are compared with results from
the experiments and from the classical lamination theory.
Chapter 4 details the experimental and numerical investigations conducted on the 2D repaired
sandwich panels. Specimens were tested under uniaxial tension loads and different scarf angles
were studied. The 2D model was used to predict the mechanical behavior of the repaired
structure until failure. This chapter is presented as the first research paper.
55
Chapter 5 discusses the parametric study conducted on the 2D repaired panels. Focus was on
the effect of different geometry parameters on the strength recovery of the repaired panels
under tensile loads. This chapter is presented as the second research paper.
Chapter 6 continues the experimental and numerical investigations on 2D repaired panels
tested under edgewise compression and four-point bending loads. This chapter is presented as
the third research paper.
Chapter 7 presents the experimental and numerical works conducted on the circular repaired
panels. Compressive and four-point bend tests were performed to determine the behavior of
the repaired specimen. Then, a 3D finite element with a progressive damage and failure for the
composite was developed to predict the stiffness and failure mode of the repaired panels. This
chapter is presented as the fourth and last research paper.
Finally, a conclusion (Chapter 8) summarizes the contributions from this research and gives
some recommendations and perspectives for future work.
56
Chapter 3.
Mechanical Characterization and Finite Element
Study of Monolithic Facesheets and Honeycomb
Core
This chapter presents the experimental results from tensile and compressive tests conducted on
plain weave (PW) and 8-harness satin (8HS) carbon/epoxy composite materials with a quasi-
isotropic lay-up. Both in-plane tensile and compressive properties were determined
experimentally. The honeycomb Nomex core was tested experimentally to determine the in-
plane and out-of-plane mechanical properties. Moreover, a 2D linear elastic ply-by-ply
through-the-thickness model of a quasi-isotropic laminate was developed using the software
Abaqus/Standard to predict the laminate elastic behavior. Results were then compared with the
classical lamination theory prediction and the experimental data to validate the finite element
model.
57
3.1 Experimental Characterization of the Facesheet Materials
3.1.1 Materials Description and Specimens Manufacturing
Materials Description
The honeycomb sandwich panels facesheets were fabricated from out-of-autoclave prepreg
made with Cycom T650-35 3k carbon fibers and 5320 epoxy resins. Two different woven
fabric architectures were used: plain weave (PW) and eight harness satin (8HS). Figure 3-1
shows the architecture pattern for the 8HS and for the PW woven fabric materials. The
composite material properties given by the manufacturer [59] are listed in Table 3-1.
Figure 3-1 Fiber architecture pattern for a) an 8HS fabric and b) a PW fabric (adapted from[60])
Table 3-1 Materials properties from Cytec [59]
Material Resin content (%) Weight (g/m2) Ply thickness (mm)
5320-PW 36 196 0.19
5320-8HS 36 370 0.38
a) b)
58
Specimens Manufacturing
A total of six plates were manufactured from PW and 8HS prepregs: four 304 x 457 mm2 plates
for tensile tests and two 153 x 203 mm2 plates of for compressive tests. The plates were
composed of 16 prepreg plies stacked as [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s for the PW
material, while for the 8HS material, eight prepreg plies with a stacking sequence of [(+45/-
45)/(0/90)/(-45/+45)/(90/0)]s was used. The panels were debulked for four hours prior to curing
using a vacuum bag (with 29 in Hg applied vacuum). Then, they were cured in an oven under
vacuum, using the cure cycle shown in Figure 3-2. After cure, specimens were cut from the
plates to desired test dimensions by water jet-milling machine. The quality of the specimens
was assessed using microscopic observation before testing as shown in Figure 3-3. No
microcracks were detected in the composite layers and porosities were quasi absent.
3.1.2 Mechanical Testing of the Laminate Used for the Skins
Tensile Tests
The PW and 8HS quasi-isotropic specimens were tested in tension, at room temperature
conditions, using an electromechanical MTS testing machine with a 100 kN load cell. A
constant crosshead displacement rate of 2 mm/min was used, in accordance with ASTM
standard D3039 [61]. Two series of specimens were prepared to determine the tensile properties
of the composite skins. Namely, five specimens were cut along the longitudinal direction of
the skin (0° direction or x-direction) and five more were cut along the transverse direction (90°
direction or y-direction) for both PW and 8HS laminates. The final specimen dimensions were
250 mm long, 25 mm wide and about 3 mm thick. To prevent failure from occurring in the
59
grips, aluminum tabs were bonded at the specimen ends. To measure the longitudinal and
transverse strains, a video-extensometer system was used. The applied stress was determined
using:
F
A (9)
where F is the recorded force during the test and A is the cross-section area of the specimen.
a. Vacuum bag arrangement for laminate curing
b. Cure cycle applied to the laminate
Figure 3-2 Vacuum bag arrangement and cure cycle used for the quasi-isotropic laminates
60
Figure 3-3 Micrographs of PW and 8HS laminate cross-sections after cure
Combined Loading Compression Tests
Combined loading compression (CLC) tests were performed according to ASTM standard
D6641 [62] at room temperature conditions. The speed of the test was set, as suggested in the
standards, to 0.5 mm/min. Rectangular test specimens were cut from the PW and 8HS laminates
along the 0°-orientation (x-direction) with a water jet-milling machine at a nominal size of 140
mm by 13 mm. The test set-up and the specimen configuration are presented in Figure 3-4. The
longitudinal strain was measured using two strain gages (CEA-06-125UW-350) bonded on
each side of the specimen. Aluminum tabs were bonded to avoid end crushing or bending
during the test. The applied compressive stress was determined using:
x
F
w t
(10)
where F is the applied load, w is the specimen width and t is the specimen thickness.
(a) 16-ply PW laminate: [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s
(b) 8-ply 8HS laminate: [(+45/-45)/(0/90)/(-45/+45)/(90/0)]s
61
Figure 3-4 CLC set-up and specimen configuration
Test Results and Interpretation
Figure 3-5 and Figure 3-6 show the tensile stress-strain responses in both the x-and y-directions
for the PW and 8HS specimens, respectively. It can be seen from these figures that the tensile
response is linear until an abrupt failure. No significant differences were observed between the
PW and the 8HS stress-strain curves for the different specimens. Moreover, all the observed
failure modes of the tensile specimens were fiber fracture, away from the grip area, as shown
in Figure 3-7.
The compressive stress-strain responses in the x-direction are shown in Figure 3-8 and Figure
3-9 for both the PW and 8HS composite specimens respectively. The compressive response
was slightly nonlinear in comparison with the tensile test results. Figure 3-10 shows the failure
mode of the specimens tested in compression. It should be noted that all the tested specimens
failed in the middle of the gage and limited bending was observed during the test. The bending
rate A (%) calculated following the ASTM standard [62] using
Strain gage 2
Strain gage 1
Tabs
3 mm
Y
X
62
11 22
11 22
A(%) 100
(11)
where ε11 is the deformation measured by strain gage 1 and ε22 is the deformation measured by
strain gage 2 didn’t exceeded 10%.
a. in the x-direction b. in the y-direction
Figure 3-5 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW
specimen tested in tension
a. in the x-direction b. in the y-direction
Figure 3-6 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]s 8HS
specimen tested in tension
63
Figure 3-7 Typical failure for specimens tested in tension in the x- and y-directions
Figure 3-8 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW
specimen tested in compression in the x-direction
Figure 3-9 Typical stress-strain curve for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]s 8HS
specimens tested in compression in the x-direction
64
Figure 3-10 Typical failure mode for specimens tested in compression in the x-direction
The test results for the PW and 8HS specimens are summarized in Table 3-2 and Table 3-3 for
the tensile and compressive tests, respectively. Despite the quasi-isotropic stacking sequence
for both PW and 8HS laminates, slight differences were observed in terms of tensile strength
and elastic modulus for the longitudinal and transverse directions. It can be observed that for
both PW and 8HS, the tensile strength in the y-direction is higher than the strength in the x-
direction. Also, the material properties varied depending on the woven architecture. The PW
laminate has a higher tensile strength in both directions, however in terms of stiffness, the 8HS
laminate was slightly stiffer. The compressive strength of the PW and 8HS specimens were
lower than the tensile strength. Also, the corresponding compressive modulus for both
materials were lower than the tensile elastic modulus.
Table 3-2 Statical analysis - tensile tests
Test
direction Material
Elastic
modulus
(GPa)
S C.V
(%)
Strength
(MPa) S
C.V
(%)
Longitudinal
x-direction
PW 45.78 2.12 4.64 649.35 37.13 5.71
8HS 45.87 1.10 2.39 611.75 27.07 4.43
Transverse
y-direction
PW 43.68 0.40 0.93 652.86 34.60 5.26
8HS 46.03 1.37 2.99 628 51.50 8.41
where: S is the standard deviation and C.V(%) is the coefficient of variation.
65
Table 3-3 Statical analysis - compressive tests
Test
direction Material
Elastic
modulus
(GPa)
S C.V
(%)
Strength
(MPa) S
C.V
(%)
Longitudinal
x-direction
PW 36.65 1.30 3.54 567.88 23.99 4.22
8HS 35.46 0.077 4.26 534.54 12.67 2.37
3.2 Mechanical Characterization of the Honeycomb Nomex Core
The core used in this study to manufacture the sandwich panels is a Nomex honeycomb core
from Euro-composites [63] with a 64 kg/m3 density. The honeycomb core has a rectangular
over-expanded cell ECA-R, as depicted in Figure 3-11. The three principal directions of a
Nomex honeycomb are:
L: the longitudinal direction, also known as the ribbon direction (single wall cell
thickness);
W: the transverse direction, which is perpendicular to the ribbon one, also known as the
double wall cell direction;
T: the through-thickness direction.
An accurate knowledge of the orthotropic honeycomb core material properties is needed when
modelling sandwich structures. The required core material properties are the in-plane Young’s
moduli EL and EW, the out-of-plane Young’s modulus ET, the in-plane shear modulus GLW, the
out-of-plane shear moduli GLT and GWT, and the three Poisson ratios νLT, νWT and νLW.
Table 3-4 summarizes the material mechanical properties given by the manufacturer [63]. The
missing elastic properties will be either determined experimentally (EL, EW and ET) and the
other part of the properties will be taken from the literature (GLW, νLT, νWT and νLW )[64]. So, to
66
determine the elastic in-plane and out-of-plane moduli, tensile and compressive tests were
performed at room temperature conditions.
Table 3-4 Mechanical properties for the ECA-R Nomex core (from [63])
Density
(Kg/m3)
Bare compression Shear
σT (MPa) GTW
(MPa)
τTW
(MPa)
GTL
(MPa) τTL (MPa)
64 4.4 55.50 1.49 21.10 0.96
Figure 3-11 Nomenclature and dimensions of a ECA-R unit cell (4.8 mm)
3.2.1 Out-of-Plane Compressive Tests
The manufactured cell-structured honeycomb was subjected to a through-thickness
compressive load at a quasi-static rate of 0.5 mm/min in accordance to ASTM standard C365
[65]. The mechanical tests were carried out at room temperature conditions using an
electromechanical MTS frame with a 10 kN load cell, as shown in Figure 3-12. A video
extensometer system was used to record the deformation of the specimen and a set of five
50x50 mm2 samples were tested. The linear zone of the compressive stress-strain response is
All dimensions are in mm
67
shown in Figure 3-13. The compressive response was slightly nonlinear, at the beginning of
the test. The calculated out-of-plane elastic compressive modulus is presented in Table 3-5.
Figure 3-12 Compressive test set-up
Table 3-5 Compressive mechanical properties for the over-expanded Nomex core
Mean S Cv (%)
ET(MPa) 185 1.34 0.72
Figure 3-13 Typical compressive stress-strain curve
68
3.2.2 In-Plane Tensile Tests
Honeycomb specimens were respectively tested in the L- and W-directions to determine the
in-plane elastic moduli EL and EW. A fixture system similar to the one recommended by the
ASTM standard C363 [66] was machined to fix the specimens and to introduce the tensile
loading at room temperature conditions. The same electromechanical MTS machine with a 10
kN load cell was used to apply a displacement at a rate of 2.5 mm/min in the W-direction and
a displacement rate of 5 mm/min in the L-direction. A set of five samples were tested in each
case. Both L and W-directions samples were 254 mm long by 128 mm wide by 19 mm thick.
The strains were recorded by using a video-extensometer. For that, targets were bonded at a
distance of 70 mm on the specimen surface. Figure 3-14 shows the specimen configuration and
the experimental set-up.
a. Specimen configuration b. Test set-up
Figure 3-14 Specimen configuration and tensile test set-up
69
Figure 3-15 presents typical tensile stress-strain curves obtained in the ribbon (Figure 3-15.a)
and in the transverse (Figure 3-15.b) directions of the honeycomb core. As the curve is non-
linear at the beginning, the stiffness in both ribbon and transverse directions were taken in the
linear part of the stress-strain curves. The calculated in-plane elastic tensile moduli are
presented in the Table 3-6. The elastic modulus in the ribbon direction is much lower than that
in the transverse one. Therefore, for the over-expanded cell honeycomb structure, the
transverse direction is stiffer than the ribbon direction and when manufacturing sandwich
panels with such a honeycomb, the W-direction should be chosen along the main loading
direction. This difference in the in-plane elastic moduli is related to the particular form of the
honeycomb cell and for a hexagonal cell, the difference between the in-plane elastic moduli is
not significant.
3.2.3 Nomex Tests Recapitulation
From the conducted in-plane and out-of-plane tests, the elastic moduli of the Nomex
honeycomb core were determined. The shear moduli and the Poisson’s ratios were taken from
the manufacturer data and the literature, respectively. Table 3-7 summarizes the mechanical
properties for the Nomex honeycomb core that will be used later in the finite element models
for the repaired sandwich panels.
Table 3-6 Tensile elastic modulus in the L-and W-directions for the over-expanded
Nomex core
EL (ribbon-direction) (MPa) EW (transverse-direction) (MPa)
Mean 0.089 30.30
S 0.0007 4.66
Cv (%) 0.79 15.40
70
Table 3-7 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R
4.8 64)
EW (MPa)
EL (MPa)
ET (MPa)
30.3a
0.089a
185a
GWL (MPa)
GWT (MPa)
GLT (MPa)
1.9b
55.5c
21.1c
νWL
νWT
νLT
0.26b
0.22b
0.022b
a experimentally measured
b estimated from [64]
c from manufacturer
a. L-direction b. W-direction
Figure 3-15 Typical tensile stress-strain curves in the ribbon (L) and transverse (W)
directions
3.3 Analytical and Finite Element Studies of the Facesheets
Mechanical Behavior
The objective of this section is to validate the predicted elastic behavior of the quasi-isotropic
laminate predicted by finite elements when modeled in the (x, z) plane finite element. The FE
model predictions will be compared with the experimental results of section 3.2 and with
predictions obtained using classical lamination theory (CLT). If the finite element modelling
71
approach is shown to be valid, the repaired sandwich coupons will later be modeled using the
same approach.
3.3.1 Classical Lamination Theory: Analytical Approach
To assess the validation of the finite element approach chosen in this work later, classic
lamination theory (CLT) was used to estimate the stiffness coefficients of the quasi-isotropic
laminate for both the PW and the 8HS materials. The material properties used for the analytical
model are summarized in Table 3-8. The in-plane tensile properties (E1, E2, G12 and ν12) were
taken from tests done by Khechen [67]. The out-of-plane properties were taken from the
literature for a similar material [68].
The relation between stresses (σi, τij) and strains (εi, γij) can be written, in the local coordinate
system (1 2 3) using:
1 11 12 16 1
2 21 22 26 2
12 61 62 66 12
Q Q Q
Q Q Q
Q Q Q
(12)
where [Q] is the stiffness matrix. The relation between the stresses and strains in the global
coordinate system (x, y, z), where x is the axis oriented at an angle θ from the fiber direction,
can then be written as:
Q
(13)
where [Q̅] is the stiffness matrix written in the (x, y, z) global coordinate system by transforming
the local stiffness matrix to the global fixed frame using:
72
1 TQ T Q T
(14)
where [T] is the transformation matrix.
Next, to calculate the equivalent stiffness of the quasi-isotropic laminate, the stiffness matrix
[A] needs to be computed via a through thickness integration that results in:
1
1
(z z )
kN
ij k k
k ij
A Q
(15)
where N is the total number of plies and zk and zk-1 are the z-coordinate of the upper and lower
surfaces of layer k. Therefore, zk-zk-1 is equal to the thickness of a single ply. The equivalent
elastic moduli, which are valid for symmetric and balanced laminates are then calculated using:
2
11 22 12
22
x
A A AE
A t
(16)
2
11 22 12
11
y
A A AE
A t
(17)
where t is the total laminate thickness.
Table 3-8 Composite materials elastic properties
E1
(GPa)
E2
(GPa)
E3
(GPa)
G12
(GPa)
G13
(GPa)
G23
(GPa) ν12 ν13 ν23
PW
material 62.66 66.93 10 4.93 4.93 4.93 0.047 0.3 0.3
8HS
material 66.27 63.34 10 5.21 5.21 5.21 0.047 0.3 0.3
73
Table 3-9 Comparison between analytical and experimental results
Material 𝐄𝐱𝐄𝐱𝐩
(GPa) 𝐄𝐱𝐂𝐋𝐓(GPa) Error (%) 𝐄𝐲
𝐄𝐱𝐩(GPa) 𝐄𝐲
𝐂𝐋𝐓(GPa) Error (%)
PW 45.78 48.49 5.58 43.68 48.49 9.92
8HS 45.87 47.39 3.20 46.03 47.39 2.87
, ,
,
(%) 100
Exp CLT
x y x y
CLT
x y
E Eerror
E
The tensile elastic moduli obtained for both PW and 8HS quasi-isotropic laminates with the
analytical approach are summarized and compared with experimental results in Table 3-9.
Differences between analytical and experimental results can be explained by the experimental
errors and manufacturing imperfections.
3.3.2 Finite element Analyses
Scarf repaired joints (circular and rectangular repair shapes) are modeled in the literature using
2D solid element models (plane strain or generalized plane strain) or full 3D finite element
models [15, 21, 68]. Rectangular repair shape corresponds generally to a 3D problem, which
can be simplified to a 2D plane strain problem for which it is easier to perform a two-
dimensional analysis of the stress distribution in the adhesive and to determine the mechanical
properties of the repaired structure. Three-dimensional (3D) models are however used to obtain
a complete understanding of the behavior of circular repairs. In this section, two main models
were developed: first, a 2D FE model was considered and then a 3D finite element model was
developed. The validity of these models was verified by comparing their predictions with CLT
and experimental results.
74
Linear Elastic Numerical Model
As explained in the preceding section, 3D rectangular repair shape can be simplified to a 2D
plane strain problem. Hence a two-dimensional (2D) linear elastic model is developed here to
predict the tensile behavior of quasi-isotropic laminates. Figure 3-16 shows the 2D plane strain
finite element model as created in the longitudinal x-z plane. As the specimen is modeled along
the longitudinal cross-section, the strain components in the y-direction are negligible:
0y xy yz (18)
i. Materials Behavior and Convention
There are different material options to model a linear elastic material in Abaqus/Standard [56]
: isotropic, orthotropic or fully anisotropic. For the studied composite facesheet, the orthotropic
option was considered. At first time, the lines and columns of the stiffness matrix, for each ply
orientation, was properly swapped to be consistent with the Abaqus convention, and then a
second time, since the thickness was modeled along the y-axis instead of the z-axis (through-
thickness convention), as explained in Figure 3-17.
Figure 3-16 Geometry of studied and simplified specimen (not to scale)
z
z
y
75
ii. Boundary Conditions and Mesh Details
The applied boundary conditions are as follow: the left edge (x=0) is fully constrained and a
displacement of 1 mm is applied at the right edge (x=L), as shown in Figure 3-18. For the finite
element mesh, two types of 2D solid elements from the Abaqus library [58] were used:
- Plane strain element with reduced integration, CPE4R,
- Generalized plane strain with incompatible mode, CPEG4I.
Each single woven ply was discretized through the thickness (z-direction) using one element
and 127 elements along the x-direction.
11 12 13 11 12 13
12 22 23
13 23 33
44
55
66
Stiffness matrix(Voigt notation) Abaqus convention Through thickness convention
0 0 0 0 0
0 0 0
0 0 0
0 0 0 0 0
0 0 0 0 0
0 0 0 0 0
C C C C C C
C C C
C C C
C
C
C
13 12
13 33 23
1
11
12 22 23
13 23 33
5
2 23 22
4466
664
55
4
5
0 0 00
0 0 00 0 0
0 0 00 0 0
0 0 0 0 00 0 0 0 0
0 0 0 0 00 0 0 0 0
0 0 0 0 00 0 0 0 0
C C C
C C CC C C
C C CC C C
CC
CC
CC
Figure 3-17 Changes in Stiffness matrix to respect modelling convention
Figure 3-18 Boundary conditions for the 2D laminate tensile test (not to scale)
76
iii. Results and Discussions
From the imposed displacement and applied force calculated by Abaqus [58], the elastic
modulus of the material can be determined. The applied stress is calculated using:
x
F
A (19)
where F is the summation of the calculated force at nodes located at x=L and A is the cross-
section area of the laminate. The strain is computed using:
0x L xx
u u
L
(20)
where ux is the displacement in the x-direction and L is the length of the laminate in the x-
direction.
The elastic modulus in the x-direction is then calculated using:
x
x
x
E
(21)
The results for the calculated elastic modulus xE using different finite elements are summarized
in Table 3-10. They are compared with the experimental and analytical results. It can be
observed that the finite element model with generalized plane strain element predicts the elastic
modulus very well. Plane strain elements overestimate the modulus by 4.76%. Therefore,
generalized plane strain elements will be used to model the elastic behavior of adherend of the
scarf-step repair in the next chapters. Since generalized plane strain elements are not available
in the ABAQUS/Explicit library [56], plane strain elements with reduced integration (CPE4R)
77
will be used for the failure analysis of scarf-step repaired panels using a 2D model. However,
those elements overestimate the stiffness of the laminate as it has been
Table 3-10 Predicted and measured elastic modulus of the quasi-isotropic laminate
PW material
Plane strain
elements
CPE4R
Generalized
plane strain
elements
CPEG4I
Experiment
CLT
xE (GPa) 50.8 46.9 45.78 48.49
observed. Hence, a correction coefficient is introduced to correlate the calculated stiffness with
the analytical one (calculated from CLT) as:
4
CLT
xcorrection CPE R
x
EC
E (22)
where is CLT
xE the elastic modulus calculated from CLT and4CPE R
xE is the elastic modulus
obtained using CPE4R finite elements.
3D Model with Progressive Damage Analysis
i. Progressive Damage Model
As the 2D finite element model will not be suitable for analyzing the mechanical behavior of
circular scarf repaired sandwich panels later, a 3D finite element model with progressive
damage for woven fabric composites was developed in Abaqus/Explicit [58]. Eight-node
continuum shell elements with reduced integration (SC8R) are used to model the quasi-
isotropic laminate. Each single ply is discretized using one element through the thickness. The
78
model relies on the built-in user’s subroutine ABQ_PLY_FABRIC for modelling the laminated
woven fabric skins (see Johnson [69] for more details on the material model).
The built-in woven fabric model is a two-dimensional mesomechanical model that
accommodate for elastic behavior coupled with damage in the warp and weft directions and
inelastic behavior for the in-plane shear. Progressive damage and failure analysis then relies on
two main failure mechanisms and one inelastic deformation mode [69]: fiber dominated failure
in tension or compression in the warp and weft directions and matrix failure in in-plane shear.
The stress-strain relation can be written in a 2D local coordinate system (1, 2) as follow:
12
1 1 111 11
2122 22
2 2 2
12 12
12 12
10
(1 d )
10
(1 d )
10 0
(1 d )
E E
E E
G
(23)
where E1, E2 are the initial undamaged elastic moduli in the wrap and weft directions, ν12 is the
principal Poisson’s ratio and G12 is the undamaged in-plane shear modulus. Variables d1, d2, d12
are the damage parameter associated with the warp-direction (1-direction), the damage
parameter associated with the weft-direction (2-direction) and the damage parameter related to
in-plane shear failure, respectively.
In order to distinguish between tension and compression behavior at a material point, the elastic
stiffness moduli E1 and E2 take their compressive or tensile values according to the sign of the
volumetric strain tr(ε)=ε11+ε22.
79
To reduce the simulation time, the mass scaling technique was used. To make sure that this
technique does not overly influence the underlying physics, the added kinetic energy for the
whole model had to be adjusted in such a way that it is less than 5% of the internal energy of
the whole system. In such cases, the mass scaling effects on the computed results was
negligible. The mechanical properties of the composite materials used for the built-in user
subroutine are summarized in Table 3-11. In case element deletion options are to be activated,
the built-in material subroutine offers different options to the user:
- The element is deleted when d1=dmax or d2=dmax under compressive or tensile load, or
when the plastic strain due to shear deformation reaches the maximum value,
- The element is deleted when d1=d2=dmax along both fiber directions, or when the plastic
strain due to shear deformation reaches the maximum value,
In this study, the first option to delete elements was used.
ii. Results and Discussions
Figure 3-19 and Figure 3-20 show the comparison between the stress-strain behavior obtained
from experimental measurements and from numerical simulations for the PW quasi-isotropic
laminate under tensile and compressive loadings. These figures indicate that the finite element
model generates results that are in a good agreement with test data in term of material stiffness.
However, one can notice that the finite element predictions underestimate the strength and
allowable maximum strain for both tensile and compressive loadings as summarized in Table
3-12.
80
It should be noted also that the failure modes are in accordance with the experimental results
reported in previous section. The major failure mode is the fiber fracture that first appears in
(0/90) and (90/0) plies and then, failure is propagated to (+45/-45) and (-45/+45) plies.
Table 3-11 Mechanical properties used for the PW composite material
E1t (GPa) E2t (GPa) G12 (GPa) ν12 3)
62.7 66.9 4.87 0.047 1500
E1c (GPa) E2c (GPa) X1t (MPa) X1
c (MPa) X2t (MPa)
49.3 48.7 999.7 772.2 875.6
X2c (MPa) S (MPa) G1t (N.mm-1) G1c (N.mm-1) G2t=G2c (N.mm-1)
789.7 38 22.5a 22.5a 22.5a
a taken from [70]
Table 3-12 Comparison between the experimental data and the finite element prediction
Tensile tests Compressive tests
Experimental FE Error (%) Experimental FE Error (%)
𝝈𝒙𝒇 (MPa) 649.35 627 3.44 567.88 530 6.67
S (MPa) 37.13 - - 23.99 - -
�̅�𝒙 (GPa) 45.78 47.24 36.65 35.74
S (GPa) 2.12 - - 1.30 - -
(%) 100FE Exp
x x
Exp
x
Error
81
Figure 3-19 Comparison of stress-strain curves between the experiment and the finite
element model for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW tested in tension in the x-
direction
Figure 3-20 Comparison of stress-strain curves between the experiment and the finite
element model for a [(+45/-45)/(0/90)/(-45/+45)/(90/0)]2s PW tested in compression in the x-
direction
82
3.4 Conclusion
In this chapter, results from in-plane tensile and compressive tests performed at room
temperature conditions for quasi-isotropic laminates for both PW and 8HS materials were
presented. For both materials, a slight variation was observed for the laminate tensile elastic
modulus in x- and y-directions. Moreover, the quasi-isotropic laminates exhibited a stiffer
modulus in tension than in compression. The elastic behavior of quasi-isotropic laminates was
also studied using the finite element analysis software Abaqus/Standard [58]. Here, different
elements were used to model the elastic behavior of the laminate. Results obtained with
different approaches were compared with the experimental values to validate the 2D developed
models. It was observed that the tensile modulus in the x-direction obtained with generalized
plane strain elements was closer to the experimental and CLT results. However, plane strain
elements over-estimated the modulus. Therefore, the generalized plane strain elements were
retained and will be used to predict the elastic behavior of scarf-step repaired sandwich
honeycomb panels in the next chapter. To model the failure behavior of repaired panels,
Abaqus/Explicit solver [58] will be used. Since generalized plane strain are not available in its
library, plane strain elements with reduced integration will be used along with a correction
coefficient to correlate the calculated stiffness with the experimental values. The progressive
damage model predicts well the behavior of the composite material until failure and the failure
modes agreed with the experimental test results.
83
Chapter 4.
Mechanical Characterization and Finite Element
Study of Monolithic Facesheets and Honeycomb
CoreArticle 1: Mechanical Performance of
Repaired Sandwich Panels: Experimental
Characterization and Finite Element Modelling
Emna Ghazali, Marie-Laure Dano, Augustin Gakwaya and Charles-Olivier Amyot
Résumé
Cet article présente les performances mécaniques des réparations par patch interne sur des
panneaux sandwich fabriqués avec des peaux en carbone-époxyde et une âme en nid d’abeille
Nomex. Tout d'abord, le comportement mécanique des panneaux intacts et réparés sous
chargement de tension est étudié. Les différents essais ont été effectués à température ambiante.
Ensuite, des analyses par éléments finis ont été effectuées pour prédire le comportement des
panneaux réparés. Deux modèles de matériau ont été développés pour le film adhésif: l'un est
élastique linéaire et le second est élastoplastique avec un critère de rupture en cisaillement.
Pour les peaux en composites tissés, un modèle élastique linéaire orthotropique a été utilisé.
Les prédictions du modèle numérique sont en accord avec les résultats expérimentaux. La
84
restitution de la contrainte à la rupture de la structure réparée augmente avec la diminution de
l'angle de biseau.
Abstract
This paper describes the static performance of adhesively bonded repairs on sandwich panels
made with carbon-epoxy composite skins and a Nomex core. First, the mechanical behavior of
pristine and repaired panels under tensile loading was studied. All tests were conducted under
room temperature conditions. Then finite element analyses were performed to predict the
repaired panel’s behavior. Two material models were developed for the adhesive film: one is
linear elastic and the second is elastic-plastic with a shear failure criterion. For the composite
skins, an orthotropic linear elastic model was used. Numerical model predictions are in good
agreement with the experimental results. It was found also that the strength recovery of the
repaired structure increases with the decrease of the scarf angle.
Keywords: Sandwich structures, bonded repair, finite element analysis, failure criteria.
4.1 Introduction
Since fiber-reinforced composite structures offer superior strength, higher stiffness, lighter
weight and greater durability [43], they are increasingly being used for primary aircraft
components traditionally made of metallic materials. However, despite their good properties,
composite airframe structures are more sensitive to impact damage, which can cause
disbonding, delamination and internal crushing. Considering their extended service life and
85
operating conditions, the extent of damage determines whether the composite components need
to be repaired or replaced. Hence, to take full advantage of their many benefits, the
improvement of their performances requires one to ensure first that these structures are durable,
repairable, and maintainable. Since fiber-reinforced composite sandwich structures are
increasingly being used in aircraft components, it has become necessary to develop effective
repair methods that will restore the component’s original design strength without
compromising its structural integrity.
Many studies have been conducted on bonded scarf and step joint repairs of monolithic
laminates. Campilho et al. [17, 19-20, 34, 71-72] have conducted a lot of work to study the
effects of different repair parameters (scarf angle, lay-up, adherend thickness) on the
performance of repaired laminated structures. They used a three-dimensional (3D) finite
element models with cohesive damage to assess the strength of external adhesive repaired patch
of Carbon Fiber Reinforced Plastic (CFRP) under tensile and compressive loads
[17, 34, 71-72].The effect of the shape geometry (single or double strap repair) on the strength
of the structure and the stress distribution have been particularly studied. They also developed
a two-dimensional (2D) finite element model for bonded repair joints [19, 20]. The main
conclusion was that the repair strength increases exponentially with the decrease of scarf angle.
Gunnion and Herszberg [21] developed 2D and 3D linear elastic parametric finite element
models to analyze stress distributions in the middle of the adhesive joint of CFRP scarf repaired
joints under tensile loading. This model allowed obtaining both shear and peel stress
distributions along the adhesive bondline. A parametric study was performed. The parameters
investigated included the adhesive and adherend thickness, the scarf angle and the stacking
86
sequence. The main conclusions are the low sensitivity of the adhesive stresses on mismatched
adherends lay-ups and the major reduction in peak stresses using an over-laminate ply covering
the full length of the specimen. Harman and Wang [14] developed an analytical technique to
optimize the shape of scarf joint between dissimilar adherends. Their technique uses a linear
variation of the scarf angle that generates a characteristic scarf profile for a given adherends
modulus ratio. Both analytical and the 2D and 3D elastic finite element modelling results
showed a dependence on the local ply orientation for peel and shear stress distributions in the
adhesive, for different ratios of adherends modulus. Charalambides et al. [16] tested
experimentally repaired CFRP joints using a 2°-scarf configuration. Distinct failure modes
were observed, as function of the environmental conditions (temperature and moisture) and the
type of load. They also performed a two-dimensional numerical analysis [15] in order to
simulate three different failure modes in scarf repairs: failure in the adhesive layer, failure
induced from delamination initiating at the corner of the overlap ply and tensile failure of the
composite adherends. Failure loads were compared with previously published experimental
work and the results were found to be in good agreement.
Several experimental studies and finite element analyses were also carried out to study the
behavior of repaired sandwich panels under different static loads. The compressive behavior
of repaired sandwich panels was investigated by Liu et al. [49]. Both experiments and finite
element analyses were conducted to study the influence of repair variables on the quality of the
repair. A progressive damage model was developed and good correlations between
experimental and numerical results were obtained. Ramantani et al. [52] developed a 2D
cohesive damage model to study the performance of repaired sandwich panels under four-point
87
bending loading. For overlap joints, they concluded that the repair strength increases as a
function of the overlap length and that the strength increases with lower scarf angles in the case
of scarf joints. Mahdi et al. [47, 48, 54] used 2D and quasi-3D finite element models to predict
the performance of both pristine and scarf repaired sandwich panels subjected to static and
fatigue four-point bend loading. Numerical analyses results showed a good correlation in terms
of stiffness prediction of both undamaged and repaired coupons. However, the ultimate load
prediction was problematic and did not show a good correlation with experiments. A series of
experimental tests were also conducted by Tomblin et al. [2, 51] to study the effects of different
process parameters on the repair quality of sandwich panels. A damage tolerance analysis on
sandwich structures was included as well. As a conclusion of their work, a methodology for
the repair process along with design tools for damage tolerance on sandwich structures were
developed. A recent study from Zhang et al. [50] was conducted to investigate the mechanical
performance of open-hole damage and circular scarf repairs in honeycomb sandwich panels
under compressive loads. A 3D finite- element model was also developed. A failure criterion
based on Hashin’s criterion with a progressive damage evolution was included for the
unidirectional composite skins. The adhesive layer was modeled using cohesive elements. The
honeycomb core was considered as an elastic-plastic material. A good agreement was found in
terms of ultimate failure load and damage shape between the experimental and numerical
results. Another finding of this work is that the structure strength increases with the decrease
of scarf angle and that the optimum number of overplies is one to reach the highest strength. In
the above-mentioned research works, focus was on scarf-scarf repair modelling using cohesive
zone elements for the adhesive bondline. However, this modelling technique is not suitable to
88
model a scarf-stepped repair configuration which is widely used in practice. Simplifying a
scarf-stepped configuration by a scarf-scarf configuration may lead to predict an inaccurate
stress distribution. Also, most of mentioned research works conduct parametric studies using
finite element analyses without correlating numerical predictions with experimental results.
Thus, the main objectives of this study is to (i) accurately model the scarf-stepped repair
configuration and to study its effects on the adhesive peel and shear stresses distribution and to
(ii) assess the numerical predictions with experimental data.
The paper presents a study conducted to investigate the behavior of co-cured bonded scarf
repair for primary structure sandwich panels under uniaxial static tensile load. Both finite
element analyses and experimental tests were performed. First, the repair procedure and the
experimental set-up are detailed. Force versus strain curves are presented and a series of
fractography images are shown to determine the failure mode and pattern in the sandwich
panels. Then, the finite element models developed using the commercial software ABAQUS
[56] are presented. Both elastic and elastic-plastic approaches were carried out to predict the
stress distribution along the adhesive bondline as the repaired sandwich panel was subjected to
tensile loading. Finally, the numerical predictions were compared with experimental results in
order to validate the finite element model.
4.2 Experimental Work
4.2.1 Repaired Sandwich Specimen Preparation
This section describes the repair procedure that was performed on the sandwich panel. The
sandwich panels used in this work are composed of an over-expanded Nomex honeycomb core
89
with a 19 mm thickness on which two four-ply carbon-epoxy skins were bonded. The skins are
made with an out-of-autoclave plain weave prepreg (CYCOM 5320 T650 PW from Cytec
Engineering Materials). The ply stacking sequence of the sandwich panels is [(+45/-
45)/(0/90)/(-45/+45)/(90/0)/core/(90/0)/(-45/+45)/(0/90)/(+45/-45)] where the 0o-direction is
the fabric warp direction and the 90o is the weft direction. The designations (+45/-45) and
(0/90) representing a single layer of woven fabric with the warp and weft fibres oriented at the
specified angles.
Therefore, the sandwich structure is symmetric. The mechanical performance of the
honeycomb sandwich panels repaired using a scarf/step adhesively bonded joint configuration
was studied. The panels were initially 711.2 mm-long and 406.4 mm-wide. The repair was
carried out on the tool facesheet. To simulate the material removal in the parent facesheet, each
prepreg ply had rectangular cut-out as shown in Figure 4-1.
The cut-outs were 712 mm-long and had a specific width such that, when stacked together, the
plies formed a drop-off. An adhesive film (Cytec FM 300-2M) was used to bond the two
facesheets to the core. Next, both skins and core were bonded and co-cured under vacuum bag
in an oven. The repair patch was manufactured as follows.
90
Figure 4-1 Parent panel dimension (not to scale).
After cure, the step shaped parent area was sanded with a 120-abrasive paper to reach the
desired scarf angle. This was followed by a surface cleaning with acetone and immediate
drying. The repair patch was prepared using the same parent prepreg material and the original
stacking sequence. The plies were cut to a specific width and stacked together to form an
overlap as shown in Figure 4-2. The overlap length Loverlap was determined from the scarf angle
α and the ply thickness tp using:
p
overlap
tL
tan (24)
Next, the adhesive film and prepreg plies were applied directly over the prepared cut-out
surface. The whole assembly was then cured under a vacuum bag in an oven according to the
manufacturer recommendations. Since the patch is across the whole panel length, the repair is
considered as 1D-scarf/step repair. In the context of the present study, only the inner facesheet
was repaired and the core was not replaced. A parametric study was conducted for the scarf
angle. Three different scarf angles were chosen (3°, 5° and 7°) to study the effect of this repair
91
variable on the repair strength. Rectangular test specimens were cut with a water jet-milling
machine at a nominal size of 335 mm by 102 mm. To prevent inadmissible ends failure and
premature failure, the specimen ends were reinforced with aluminum inserts and aluminum
tabs.
Figure 4-2 1D scarf/step repair configuration (not to scale).
4.2.2 Tensile tests procedure
As a next step, the repaired panels were tested in uniaxial tension using an electromechanical
‘MTS’ testing machine at a constant crosshead rate of 1 mm/min. A homemade tensile test
fixture, inspired from the one used by Tomblin et al. [2], as shown in Figure 4-3, was used for
these tests. The top and bottom grips were connected to the load cell via a universal joint. These
tests were performed in order to compare the mechanical performance of repaired panels with
pristine panels. Table 4-1 summarizes the test matrix followed for each configuration.
Core
Bag face
Parent
Adhesive
Loverlap
Tool face
tp
α (°)
Z
X
Parent Patch
92
The surface of the tool facesheet was prepared for measurement with a 3D digital image
correlation (DIC) system (Aramis by Gom [73]). The DIC software allows determining the full
in-plane and out-of-plane displacements and the strain field on the specimen surface during
testing. A video extensometer was used in order to measure the strain on the bag facesheet. The
strain measured by the DIC system was averaged on an area taken in the middle of the specimen
to obtain a single value that can be compared to the strain measured by the video extensometer.
For the repaired specimens, the strain was averaged in the middle of the patch.
4.2.3 Experimental Results
The results of the static tensile tests performed at ambient temperature on the pristine and
repaired sandwich specimens are presented in Figure 4-4 and Figure 4-5. Figure 4-4 (a) and
Figure 4-4 (b) present the load versus strain measured on the tool facesheet with the DIC system
for the pristine and the 3o-repaired specimens, respectively. As can be observed, the load-strain
behavior is mostly linear until failure for both the pristine and the 3°-repaired specimens. For
the 5°- and 7°-repaired specimens, a similar trend for the load-strain curves was also observed.
Figure 4-5 (a) and Figure 4-5 (b) present the load versus strains measured on both tool and bag
facesheets for one pristine and one 3o-repaired specimen, respectively. The uniform load
distribution in both facesheets can be assessed by the similarity in strains measured by the DIC
system and the video extensometer. For the 5°- and 7°-repaired panels, a similar behavior was
observed. Figure 4-6 compares the experimental failure load for the three investigated scarf
angles. As can be observed, the variation of scarf angle has no major effect on the ultimate
load. When the angle is equal to 3°, the ultimate failure load is about 55% of the pristine value.
93
The strength recovery for this sandwich repair configuration is quite low. Using an overply
could be beneficial to improve the strength of the repaired sandwich panel.
Table 4-1 Test matrix.
Skin material Pristine Specimens Repaired Specimens
3° 5° 7°
Plain weave 3 3 3 3
Figure 4-3 Tensile test set-up.
a. Pristine panels b. 3°-repaired panels
94
Figure 4-4 Axial load-strain curves obtained for the pristine and 3-repaired sandwich
specimens (strains measured by DIC on the tool facesheet).
a. Pristine panel b. 3°-repaired panel
Figure 4-5 Comparison of the axial load-strain curves obtained on both facesheets of the
sandwich specimens.
Figure 4-6 Tensile failure load of the pristine and repaired sandwich specimens.
Strain measurement comparison
42.50 kN 42.09 kN 41.85 kN
82.86 kN
95
4.2.4 Damage Mode and Fractography Studies
The fractured surfaces of pristine and repaired panels are shown in Figure 4-7 and Figure 4-8.
Figure 4-7 shows the ruptured facesheets of a pristine specimen. Damage occurred in both
facesheets far from the loaded ends. The failure mechanism was similar for all pristine panels.
Failure seems to be due to rupture of the skin in tension. To confirm this hypothesis, the
ultimate stress in the skin was evaluated using:
2
ultult tensiletensile
f
P
t b (25)
where tf is the facesheet thickness, b is the specimen width and ult
tensileP is the ultimate tensile
load and compared with the strength of a quasi-isotropic [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)]2s
laminate made with the same prepreg (Table 4-2). The ultimate stress in the sandwich skin is
about 87% of the quasi-isotropic laminate strength, which corroborates that the sandwich
failure mode is dominated by skin failure.
Figure 4-8shows the ruptured facesheet for the 3°-repaired panels for which failure occurred
mainly in one of the two scarf zones.
Table 4-2 Comparison of the ultimate stress between the sandwich skin and a [(+45/-45)/
(0/90)/ (-45/+45)/ (90/0)]2s quasi-isotropic laminate made from the same PW prepreg [74]
Pristine
sandwich
Quasi-isotropic
laminate
σult [MPa] Mean 536 618
S 27 19
96
Figure 4-7 Failure mode of pristine panels.
Figure 4-8 Failure mode for the 3°-repaired sandwich panels.
The quality of the pristine and of the repaired sandwich specimens was assessed using
microscopic observation before testing. As shown in Figure 4-9 (a), the pristine specimen
contains a few macro pores in the composite layers. The repaired sandwich specimen (Figure
4-9 (b)) has also some macro porosities in the composite layers. However, the repair bondline
has a very low porosity level. Cross-sections of tested repaired specimens were also examined
using optical microscopy to determine the failure modes and patterns. Figure 4-10 shows the
Failure
zone Tool faceshee
t
Bag
facesheet
Parent
Patch
Failure zone/ scarf zone
102 mm
102 mm
97
fractography images for a 3°-repaired sandwich specimen. Failure seems to be due to adhesive
and cohesive failure of the adhesive film. The adhesive is fractured along the patch side, near
the stepped plies and not on the parent side. This can be explained by the high stress
concentration in this zone. Also, macrocracks were observed in the composite plies along the
patch side.
Figure 4-9 Micrograph of the cross-section of the (a) pristine specimen, (b) repaired
sandwich specimen before testing.
Figure 4-10 Micrograph of the 3°-repaired sandwich specimen cross-section after failure.
(b)
5000 μm
Patch Parent
Adhesive bondline Macro porosity
(a)
Cohesive failure
Crack/porosity Patch laminate
6000μm
800μm
Adhesive failure
3000 μm
98
4.3 Numerical Simulation
4.3.1 Model Description
The finite element software packages ABAQUS/Standard and ABAQUS/Explicit were used to
study the response of the sandwich panels under tensile loading. Two different configurations
were studied: one corresponds to the pristine specimen and the other to the repaired specimen.
The repair joint was considered as a symmetric and plane strain problem. As such, only half
the longitudinal cross-section was modeled. The panel were 165 mm-long, 102 mm-wide and
20.5 mm-thick. The boundary conditions are defined as follow. On the left edge, the total
displacement, as measured from the experiment, was applied and, on the right edge, symmetric
boundary conditions were imposed as depicted in Figure 4-11.
Each woven ply and the adhesive film were discretized through the thickness using one and
four elements, respectively. The adhesive film along the joint as well as between the two skins
and the core was modelled. The Nomex honeycomb core was also discretized through the
thickness using 20 elements.
Two types of analyses were conducted. First, an elastic analysis with an isotropic elastic
behavior of the adhesive was performed in order to determine the stress distribution along the
bondline. ABAQUS/Standard was used to conduct this analysis. The objective of the second
analysis was to predict the mechanical behavior until failure of the repaired specimens. This
analysis took into account plastic deformation and shear failure for the adhesive and was
conducted using ABAQUS/Explicit. Two types of continuum elements were used for the
elastic finite element analysis: generalized plane strain element with incompatible modes
99
(CPEG4I) and plane strain element with reduced integration (CPE4R), both from the
ABAQUS/Standard Library. The mechanical properties of the composite materials used for the
sandwich panels are summarized in Table 4-3. The mechanical properties of the adhesive film
are indicated in Table 4-4 and the elastic properties of the Nomex honeycomb core are listed
in Table 4-5. A shear failure criterion was used to predict the failure in the adhesive film.
Figure 4-11 Description of the boundary conditions.
Table 4-3 Mechanical properties of the plain weave material.
E1 [GPa] E2 [GPa] E3 [GPa] G12[GPa] ν12 tp [mm]
64.6a 64.6a 10b 4.9a 0.047a 0.19 a experimentally measured
bassumed
Table 4-4 Mechanical properties of the FM300-2M adhesivea.
E[GPa] G [GPa] ν τy [MPa]
2.024 0.770 0.3 30
a determined from experimental data [75]
ux= 1mm u
x= 0
uRy
=uRz
=0
z x
100
Table 4-5 Mechanical properties of the Nomex honeycomb core
EW (MPa)
EL (MPa)
ET (MPa)
30.3a
0.089a
185a
GWL (MPa)
GWT (MPa)
GLT (MPa)
1.9b
55.5c
21.1c
νWL
νWT
νLT
0.26b
0.22b
0.022b
a experimentally measured
b taken from published literature [64]
c provided in material sheets
4.3.2 Linear Elastic Numerical Model
First, the effect of the element choice (CPEG4I versus CPE4R) on the stiffness prediction will
be investigated. Next, the influence of various scarf angles, namely 3°, 5° and 7°, for a scarf-
step bonded repair will be studied. The results of a 2D linear elastic, ply-by-ply and through-
the-thickness model will be presented for these three different geometric angle configurations.
The effect of this parameter on the shear and peel stress distributions along the bondline in the
middle of the adhesive will also be investigated.
Table 4-6 presents the stiffness of the pristine panels predicted using generalized plane strain
elements (CPEG4I) and plane strain elements (CPE4R). For comparison purposes, the stiffness
predicted using classical lamination theory (CLT) and the stiffness measured experimentally
are also indicated. As shown in Table 4-6, the stiffness of pristine panels predicted using plane
strain elements are overestimated by 10 % whereas the stiffness predicted using generalized
plane strain elements is very close to the experimental and CLT results. Therefore, generalized
plane strain elements will be used to model the adherends of the scarf-step repair.
In order to better understand the behavior of the repair joints, it is crucial to investigate the
stresses distribution in the weak point of the joint, which is the adhesive. Stresses in the
adhesive were extracted at nodes along a line taken in the middle of the adhesive layer as shown
101
in Figure 4-12. Figure 4-13 and Figure 4-14 compare the shear and peel stresses distributions
along the normalized bondline for the three scarf angles. As expected, stress peaks are
observed. Unlike homogeneous adherends, the stress distribution in laminated joints varies
from one ply to another and peaks occur in the vicinity of the (0/90) and (90/0) plies. Shear
stresses are much higher in magnitude than peel stresses except at the first (0/90) ply. The
maximum shear stress even exceeds the adhesive shear yield stress (given in Table 4-4).
Therefore, the adhesive begins to plastically deform. The repair joint with a 3°-scarf angle
shows the lowest shear stress values compared to 5°- and 7°-scarf repairs. The highest stress
peaks are observed for the 7°-scarf repair. Therefore, failure would be more likely to occur at
a lower load for a 5°- or 7°-scarf joint than for a 3°-scarf repair.
Table 4-6 Stiffness prediction of pristine panels.
Plane stain element
(CPE4R)
Generalized plane strain
element (CPEG4I) Experiment
CLT
𝐸𝑥̅̅ ̅ [GPa] 52.64 47.37 47.87 47.19
Figure 4-12 Line and local coordinate system used to extract peel and shear stresses
Middle of the
bondline 2
1
102
Figure 4-13 Shear stress distribution along the bondline.
Figure 4-14 Peel stress distribution along the bondline.
4.3.3 Non-linear Elastic Plastic Model
As the adhesive begins to plastically deform, it is important to implement the elastic-plastic
behavior of the adhesive film and a shear failure criterion. In the literature, different plasticity
models have been used [35–37]. The Drucker-Prager plasticity model [35, 37] is well suited
for describing pressure dependent plasticity materials such as epoxy adhesives and gives results
103
that reproduce accurately experimental strain hardening data [35]. However, this model
requires much more material parameters for plasticity than a classical metal plasticity model
based on von Mises criterion. Moreover, as observed by Shih-Pin [37], Abaqus computation
based on Drucker-Prager plasticity model presents convergence difficulty, requires a finer
mesh and therefore longer computation time than for a von Mises plasticity model. Shih-Pin
[37] observed also that as far as ultimate shear failure is concerned, classical metal plasticity
model leads to almost the same results with less numerical issue as a Drucker-Prager plasticity
model. For these reasons, it was decided in this study to use a von Mises plasticity model
combined with a shear failure criterion to assess the strength of the adhesive joint in the scarf-
stepped repair.
The plasticity model uses the von Mises yield surface with an associated plastic flow. The von
Mises criterion interprets yielding as a purely shear deformation process which occurs when
the effective shear stress e reaches a critical value o [38]. This effective stress is defined in
terms of stresses by:
2 2 2
1/22 2 21
62
xy yze x y zy z xz x
(26)
Similarly, the effective plastic strain is defined in terms of plastic strains by:
2 2 2 2 2
1/
2
22
23
x y y z z x xy yz xz
p
e
(27)
104
The plastic properties of the adhesive were determined from a ASTM D5656 Thick Adherend
Shear Test (TAST) [75]. During the test, the adhesive is supposed to be subjected to pure shear
stress. Therefore, the effective stress e is related to the shear stress by
eσ = 3 xy (28)
In case of a 2D plane strain analysis, the effective plastic strain equation under pure shear
becomes:
3
p
xyp
e
(29)
Once the initial yield shear stress (y) is reached, the equivalent plastic strain and effective
stress were calculated from the test data using eqs. (28) and (29). The hardening input data
required to model the plasticity of the adhesive film in ABAQUS are given in Table 4-7. The
data are based on experimental results from a ASTM D5656 Thick Adherend Shear Test
(TAST) [75]. From the ASTM D5656 test results, the shear yield stress and the elastic shear
modulus were determined. A shear failure criterion was also associated with the von Mises
yield criterion to predict the failure of the adhesive. This criterion is based on the value of the
equivalent plastic strain at element integration points. Failure is assumed to occur when the
damage parameter w exceeds one [36] . This damage parameter is defined as follows:
pl
pl
f
w
(30)
105
where 𝜀̅𝑝𝑙 is the equivalent plastic strain and designated as PEEQ in ABAQUS/Explicit, ∆𝜀̅𝑝𝑙 is
the increment of PEEQ and 𝜀�̅�𝑝𝑙
is the plastic strain at failure. When the shear failure criterion
is reached at an element integration point, the material is assumed to fail at this point and the
stress components are set to zero. The element is deleted from the mesh when the material
failure is detected at all integration points.
Since the generalized plane strain elements are not available in the ABAQUS/Explicit library,
plane strain elements with reduced integration (CPE4R) were used for the analysis. However,
those elements overestimate the stiffness of the sandwich panel as it has been demonstrated in
the previous section. Hence, a correction coefficient was used to adjust the calculated stiffness.
This correlation coefficient is defined as:
4
CLTcorrection
CPE R
EC
E (31)
where ECPEG4I is the elastic modulus predicted using CPEG4I elements and ECPE4R is the elastic
modulus numerically obtained using CPE4R elements.
The shear strain, 𝛾, was converted into the plastic shear strain, 𝛾𝑝, using:
p
G
(32)
where G is the shear modulus of the adhesive.
106
4.3.4 Numerical Results and Discussion
Numerical simulations have been performed to predict the mechanical behavior of the repaired
sandwich panels and compared to experimental results. Figure 4-15 shows a comparison
between the experimental results and the numerical results obtained with Abaqus/Explicit for
the 3°-repaired configuration. As can be seen from the curves, experimental and numerical
results are fairly similar. This indicates that the finite element model can simulate the behavior
of the repaired sandwich panels accurately. To further study the influence of repair parameters
(i.e. overlap length on tensile strength), finite element analyses were conducted using models
with different scarf angles. Figure 4-16 shows the evolution of the failure load (Pf) and
efficiency (η) with the increase of the scarf angle. Experimental results presented in Figure 4-6
are also added for comparison. For scarf angles between 3° and 7°, Pf and η decrease only very
slightly. These predictions corroborate very well the failure loads obtained experimentally. For
scarf angles below 3°, these two parameters increase exponentially with angle reduction. For a
1.5°-scarf angle, the efficiency reaches 64 %. However, for scarf angles over 7°, these
parameters decrease drastically. This phenomenon is related to the decrease of the overlap
length with the increase of angle, which induces the peel and shear stresses peaks to increase
at the bondline ends and at the neighborhood of the stepped plies.
Table 4-7 Hardening data input.
Yield stress, σe [MPa] Plastic strain, εpe [-]
55 0
60 0.0017
70 0.0084
75 0.015
80 0.032
107
82 0.057
84 0.12
Figure 4-15 Finite element prediction versus experiment results for the 3°-repaired
sandwich panels.
Figure 4-16 Failure load and efficiency (η=𝑃𝑟𝑒𝑝𝑎𝑖𝑟
𝑓
𝑃𝑢𝑛𝑑𝑎𝑚𝑎𝑔𝑒𝑑𝑓 𝑥100) for different scarf-step
angles.
η (%
)
108
4.4 Conclusions
This study investigated bonded repairs in sandwich panels made with honeycomb core and out-
of-autoclave prepreg carbon-epoxy skins. Experimental tests were carried out to investigate the
tensile behavior of both pristine and repaired panels. Experimental results indicate that the
repair configuration studied in the paper recovers only 55% of the static mechanical strength
of the pristine panels for a 3°-scarf-step repair at room temperature conditions. The common
failure mode for all tested repaired specimens was the failure of the adhesive joint. Both
adhesive and cohesive failure were observed experimentally.
A 2D finite element model for the sandwich panel is proposed in the paper. Good agreement
between stiffness and strength predictions and experimental results confirmed that the
numerical model provides an effective analysis tool for the mechanical behavior prediction of
repaired sandwich panels. Also, the finite element models show that the tensile strength
increases as the scarf angle decreases due to the decrease of both peel and shear stresses peaks
in the adhesive bondline.
ACKNOWLEDGEMENTS
The author would like to thank the Natural Sciences and Engineering Research Council of
Canada (NSERC), the Consortium for Research and Innovation in Aerospace in Quebec
(CRIAQ), the National Research Council Canada (NRC), Bombardier Aerospace and L3-MAS
for funding, technical support and materials.
109
Chapter 5.
Article 2: Parametric Study of Stepped-Scarf
Bonded Joints in Repaired Honeycomb Sandwich
Composite Panels
Emna Ghazali, Marie-Laure Dano and Augustin Gakwaya
Résumé
Les réparations avec patch interne de type escalier-biseau de structures sandwich peuvent offrir
une bonne alternative plus facile à réaliser que les réparations avec patch interne de type biseau.
Cet article étudie l'effet de différents paramètres géométriques sur la distribution des
contraintes dans le joint de colle ainsi que la contrainte à la rupture de la structure réparée. Des
modèles par éléments finis élastiques linéaires et élastoplastiques non linéaires ont été
développés pour mener une étude paramétrique pourtant sur l'angle du biseau, le nombre de
plis et l'addition d'un extra-pli. Les résultats montrent que les réparations de type escalier-
biseau ont une sensibilité importante à l'épaisseur des peaux. L'utilisation d'un extra-pli fournit
une protection aux extrémités libres de l'adhésif et augmente la résistance de la structure
sandwiche réparée.
110
Abstract
Stepped-scarf patch repairs of honeycomb sandwich structures can offer a good alternative easier
to perform than tapered scarf repairs. This study investigates the effect of different stepped-scarf
joint geometrical parameters on stress distribution in the adhesive bondline and on the failure load
of repaired composite sandwich panels. Both linear elastic and non-linear elastoplastic with failure
criterion analyses were conducted to perform a parametric study focusing on scarf angle, number
of plies and the addition of an overply. Results show that stepped-scarf joints exhibit an important
sensitivity to the thickness of repaired skins. The use of an overply provides protection to the free
ends of the adhesive joint and increases the strength recovery of the repaired sandwich structure.
Keywords: Sandwich structures, bonded repair, finite element analysis, parametric study.
5.1 Introduction
Adhesively bonded joints are increasingly being used nowadays in different industry fields and
especially in the aerospace industry for its advantages in maintaining aerodynamic performance
and in ensuring uniform stress distribution. However, to insure the highest strength recovery of
the structure, different parameters such as the scarf angle, the lay-up or the adherend thickness
should be taken into account in order to design an optimal repair.
Many studies have been conducted on bonded scarf and stepped joint repairs of monolithic
laminates. Campilho et al. [17, 20, 34, 71-72] have conducted a lot of work to study the effects of
different repair parameters (scarf angle, lay-up, adherend thickness) on the performance of tapered
scarf repaired laminated structures. They used a three-dimensional (3D) finite element models
with cohesive damage to assess the strength of external adhesive repaired patch of Carbon Fiber
111
Reinforced Plastic (CFRP) under tensile and compressive loads [17, 20, 34]. The effect of the
shape geometry (single or double strap repair) on the strength of the structure and the stress
distribution have been particularly studied. They also developed a two-dimensional (2D) finite-
element model for bonded scarf repair joints[19-20]. The main conclusion was that the repair
strength increases exponentially with the decrease of scarf angle. Gunnion and Herszberg [21]
developed2D and 3D linear elastic parametric finite element models to analyse stress distributions
in the middle of the adhesive joint of CFRP scarf repaired joints under tensile loading. Their model
allowed obtaining both shear and peel stress distributions along the adhesive bondline. A
parametric study was performed. The parameters investigated included the adhesive and
adherends thickness, the scarf angle and the stacking sequence. Their main conclusions are the
low sensitivity of the adhesive stresses to mismatched adherends lay-ups and the major decrease
in peak stresses using an over-laminate ply covering the full length of the specimen.
Whereas bonded repairs of solid composite laminates have been extensively studied through
analytical, numerical or experimental works, investigations on bonded repairs of composite
sandwich structures are very limited in the literature. However, conclusions drawn for solid
composite laminates repairs are not necessarily applicable to composite sandwich repairs and it is
therefore important to pursue research efforts in this area. So far, a few experimental studies and
finite-element analyses were carried out to study the behaviour of repaired sandwich panels under
different static loads.
Mahdi et al. [47, 54] used 2D and quasi-3D finite-element models to predict the performance of
both pristine and tapered scarf repaired sandwich beams subjected to static four-point bending
loading. Numerical analyses results showed a good correlation in terms of stiffness prediction of
112
both undamaged and repaired specimens. However, the failure load prediction was problematic
and did not show a good correlation with experiments. The failure load of the beam was predicted
using Tsai-Hill failure criterion and was based on the composite first ply failure. The model was
not able to capture the complex failure modes of the repaired beams. In particular, adhesive failure
was not taken into account.
Ramantani et al. [52] developed a 2D cohesive damage model to study the performance of overlap
and tapered scarf repaired sandwich beams under four-point bending loading. The sandwich skins
and patches were constituted of 0o unidirectional laminates. The effects of different parameters
(overlap length and patch thickness for the overlap repair and scarf angle for the tapered scarf
repair) were discussed. For overlap repairs, they concluded that the repair strength increases as a
function of the overlap length and that the strength increases with lower scarf angles in the case
of scarf repairs.
A series of experimental tests were also conducted by Tomblin et al. [2, 51] to study the effects of
different process parameters (scarf angle, core cell size and repair material) on the repair quality
of sandwich panels. Two repair methods were tested: a wet-lay-up repair procedure and a prepreg
repair procedure using plain weave carbon-epoxy prepreg. A damage tolerance analysis on
sandwich structures was included as well. As a conclusion of their work, a methodology for the
repair process along with designing tools for damage tolerance on sandwich structures were
developed.
The compressive behaviour of sandwich panels with circular tapered scarf repair was investigated
by Liu et al. [49]. Both experiments and finite element analyses were conducted to study the
influence of repair variables (scarf angle and cure temperature) on the repair quality. A progressive
113
damage model was developed for the composite plies and a cohesive element model was used for
the adhesive film. Good correlation between experimental and numerical results were obtained
for different scarf angles. A recent study by Zhang et al. [50] investigated the mechanical
performance of open-hole damage and circular scarf repaired honeycomb sandwich panels under
compressive loads. A 3D finite-element model was also developed. A failure criterion based on
Hashin’s criterion with a progressive damage evolution was included for the unidirectional fiber-
reinforced composite plies used for the skins. The adhesive layer was modelled using cohesive
elements. The honeycomb core was considered as an elastic-plastic material. A good agreement
was found in terms of failure load and damage shape between the experimental and numerical
results. The influence of the scarf angle and the number of 0o-overplies was studied. Conclusions
of the study were that the structure strength increases with the decrease of scarf angle and that the
optimum number of overplies is one to reach the highest strength.
In the above-mentioned research works on bonded repairs of composite sandwich structures, focus
was on scarf-scarf repair modelling using cohesive zone elements for the adhesive bondline.
However, this modelling technique is not suitable to model a stepped-scarf repair configuration,
which is commonly used in practice. Simplifying a stepped-scarf configuration by a scarf-scarf
configuration may lead to predict inaccurate stress distributions. Also, the parametric studies that
were so far conducted on scarf repaired sandwich structures were limited to investigate the effect
of scarf angle [50, 52] and the number of overplies [50] and were not validated with experimental
results.
The aim of the research work presented in this paper is to provide an in-depth understanding
of the tensile behavior of bonded stepped-scarf repaired composite sandwich structures through
114
finite-element analyses and experiments. As in previous studies encountered in literature for
repairs in solid composite laminates, a parametric study is conducted to determine the influence
of the scarf angle, the number of plies, and the use of an overply (overlap length) on the strength
recovery of repaired composite sandwich panels. First, a 2D elastic linear model is used to
determine the peel and shear stress distributions along the bondline. Then, the 2D model is
modified and an elastic-plastic model for the adhesive is taken into account to determine the
failure stress of different repair configurations. A comparison of the baseline model predictions
with experimental results is also presented.
5.2 Finite Element Model Description
The finite-element model used for the parametric study is based on a model developed by the
authors and that is described in details in [76]. The developed model has the particularity to model
the adhesive film using solid elements and to take into account its elastic-plastic behavior that has
been experimentally determined. The model has already been presented and validated using
experimental results in [76]. Here, the goal is to use the developed model to further study repairs
of composite sandwich structures by investigating the effects of different repair configuration
parameters. The following subsections describe the model geometry, the boundary conditions, the
finite-element mesh and the materials models used in the finite element analysis of stepped-scarf
repaired honeycomb sandwich panels under tensile loading.
5.2.1 Model Geometry and Material System Description
The repaired sandwich panels considered in this study have a double stepped-scarf joint, as
shown in Figure 5-1. The repair is located on the tool facesheet. The panels are 335 mm long,
115
102 mm wide and 20.52 mm thick. They are composed of an over-expanded Nomex
honeycomb core with a 19 mm thickness on which two four-ply carbon-epoxy skins were
bonded. The skin is made with an out-of-autoclave plain weave prepreg (CYCOM 5320 T650
PW from Cytec Engineering Materials) with a 0.19 mm thickness. The ply stacking sequence
for the inner facesheet, also called the tool facesheet, is a [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)].
The outer facesheet, also called the bag facesheet, has the same lay-up as the inner one. The
patch repair has also the same lay-up as the parent structure. The skin 0°-direction is aligned
with the x-direction. The ribbon direction (L-direction) of the Nomex core is along the y-
direction. The repair patch is bonded to the parent structure by an adhesive film (FM 300-2M
from Cytec) with a 0.25 mm thickness, placed along the scarf and under the patch. Only half
of the longitudinal cross-section was modeled (Figure 5-2) using a two-dimensional model with
plane strain conditions.
Figure 5-1 Configuration of the double scarf-stepped repair joint (not to scale).
102 mm
116
Figure 5-2 Symmetric cross-section of the double scarf-stepped repaired sandwich panel
(not to scale).
5.2.2 Boundary Conditions and Finite Element Mesh Details
Looking at Figure 5-2, the boundary conditions are defined as follow. On the left edge (x=L),
a total displacement, as measured from the experiment [76], was applied and, on the right edge
(x=0), symmetric boundary conditions were imposed. Each single woven ply and the adhesive
film were discretized through the thickness using one and four elements, respectively.
The adhesive film along the joint as well as between the two skins and the core was modelled
too. The Nomex honeycomb core was discretized through thickness using five elements. Two
types of continuum elements were used for the finite element analyses. Generalized plane strain
elements with incompatible modes (CPEG4I) were used for analyses carried out with
ABAQUS/Standard. This element type was selected because it was the most appropriate to
accurately predict the adherend stiffness [76]. However, since this element type is not available
X = L X = 0
117
in the ABAQUS/Explicit library, plane strain elements with reduced integration (CPE4R) were
used for analyses carried out with ABAQUS/Explicit [56].
5.2.3 Materials Models
The finite element software packages ABAQUS/Standard and ABAQUS/Explicit [56] were used
to study the mechanical response of the repaired sandwich panels under tensile loading. Two types
of analysis were conducted. First, an elastic analysis with isotropic elastic behavior of the adhesive
and orthotropic elastic material for the composite layers was performed in order to determine the
shear and peel stress distributions along the bondline of the stepped-scarf joint. The second
analysis took into account von Mises plasticity with a shear failure criterion for the adhesive film
to predict the mechanical behavior until failure of the repaired sandwich panel. The non-linear
plastic model is described in details in [76]. A failure criterion based on maximum fiber strain was
used to predict failure of the composite skins. For both analyses, the honeycomb core was
considered as an equivalent orthotropic elastic material. The mechanical properties of the
composite material used for the sandwich panel skins are summarized in Table 5-1. The
mechanical properties of the adhesive film are indicated in Table 5-2 and the elastic properties of
the Nomex honeycomb core are listed in Table 5-3.
Table 5-1 Mechanical properties of the plain weave composite material
E1 (GPa)
E2 (GPa)
E3 (GPa)
64.6a
64.6a
10b
G12 (GPa)
G13 (GPa)
G23 (GPa)
4.9a
4.9b
4.9b
ν12
ν13
ν23
0.047a
0.3b
0.3b
a experimentally measured
b assumed
118
Table 5-2 Mechanical properties of the FM300-2M adhesive
E
(GPa)
G
(GPa) ν
τy
(MPa)
2.024 0.770 0.3 30
Table 5-3 Mechanical properties of the Nomex honeycomb core
EW (MPa)
EL (MPa)
ET (MPa)
30.3a
0.089a
185a
GWL (MPa)
GWT (MPa)
GLT (MPa)
1.9b
55.5c
21.1c
WL
WT
LT
0.26b
0.22b
0.022b
a experimentally measured
b taken from published literature [64]
c provided in material sheets [63]
5.3 Parametric Study
The finite element model was used to conduct a parametric study to provide an in-depth
understanding of the tensile behavior of bonded stepped-scarf repaired composite sandwich
structure. This loading configuration was selected because some experimental results were
available to validate the model predictions. The geometrical design parameters investigated are
the scarf angle (α), the number of plies (N) and the overlap length of the overply (Lo). These
parameters are listed in Table 5-4 and the baseline values are shown in
Table 5-5. With the exception of the scarf angle [50, 52], the effect of these parameters on
composite sandwich repairs have so far not being investigated.
The main objective of this study is to investigate the influence of these parameters on the shear
and peel stress distributions along the bondline of the stepped-scarf joint. For that, shear and
119
peel stresses were extracted from the same nodes along a line in the middle of the bondline, as
depicted in Figure 5-3. The shear stress (τ12) is tangent to the bondline 1-direction 1 of the local
1-2 plane and the peel stress (σ22) is along the 2-direction. To allow comparison of the relative
magnitude, the shear and peel stresses were normalized by the stress σx applied in the global x-
direction as follow:
12 1000x
(33)
22 1000x
(34)
The second objective of this study is to determine the strength of the repaired sandwich panel and
to compare it with the one of the pristine panel. The strength was evaluated using:
2
ff
f
P
bt (35)
where Pf is the failure load, tf is the facesheet thickness and b is the panel width.
Figure 5-3 Line and local coordinate system to extract peel and shear stresses in the
adhesive joint.
Table 5-4 Parametric model details
Parameter Value
Scarf angle, α (°) 1.5-15
Number of plies, N 2, 4 and 8
Overply lay-up (+45/-45)
120
Overlap length, Lo (mm) 0-5-10-15
Table 5-5 Baseline model values
Parameter Value
Scarf angle α (°) 3°
Adhesive thickness, ta (mm) 0.25
Ply thickness, tp (mm) 0.19
Number of plies, N 4
Overply lay-up no overply
Overlap length, Lo (mm) no overply
5.4 Results
Effect of the Scarf Angle
In this section, the influence of various scarf angles was studied by varying α from 1.5° to 15o
while other parameters were kept the same as for the baseline model. First, the effect on the
shear and peel stress distributions along the adhesive bondline is discussed. Then, to further
study the influence of the scarf angle on the tensile strength, finite element analyses with failure
criteria were conducted using geometric models with different scarf angles. The failure stress
variation as a function of the scarf angle is presented.
i. Shear and Peel Stress Distributions along the Bondline
Figure 5-4 (a) and Figure 5-4 (b) compare the normalized shear and peel stresses as a function
of the normalized distance along the bondline for different scarf angles, respectively. As
expected, the stress distribution varies from one ply to another due to the mismatch in ply
properties and peak stresses occur in the vicinity of (0/90) plies. It can also be seen that the
bondline stresses are very sensitive to the scarf angle variation. As the scarf angle decreases,
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the peel and shear stress peaks decrease. These results are in accordance with conclusions of
previous works [21] conducted on monolithic composite repairs.
a. Shear stress distribution along the middle of the bondline.
b. Peel stress distribution along the middle of the bondline.
Figure 5-4 Shear and peel stress distributions along the adhesive bondline for different
scarf angles.
(+45/-45) (0/90) (-45/+45) (90/0)
(+45/-45) (0/90) (-45/+45) (90/0)
122
ii. Failure load
Figure 5-5 presents the variation of the repair strength with the increase of scarf angle.
Experimental results [76] are also added for comparison and validation of the model
predictions. For scarf angles between 3° and 7°, the strength decreases only very slightly. These
predictions corroborate very well the strengths obtained experimentally. For scarf angles below
3°, the strength increases with angle reduction. The highest strength is obtained for the 1.5°
scarf angle and reaches 62.7 % of the pristine panel strength. For scarf angles over 7°, the
strength decreases drastically. This phenomenon is related to the decrease of the bondline
length with the increase of the angle. This induces the shear and peel peak stresses to increase
at the bondline ends and at the neighbourhood of the stepped plies. For the failure mode, the
finite-element analysis predicts that failure occurs in the adhesive film for angles from 1.5° to
15°. The same failure mode was observed experimentally for angles from 3° to 7°.
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Figure 5-5 Repair failure stress for different scarf angles.
Effect of the Overply
Here, the effect of adding a (+45/-45) overply was investigated using the 3°-scarf joint model
with the baseline parameters. The overply is made with the same plain weave composite
material as the parent and the patch plies and has therefore the same thickness, tp. The overlap
length (Lo), defined in Figure 2, varied from 0 mm to 15 mm. The same boundary conditions
and displacement were applied as for the baseline model.
i. Shear and peel stress distributions along the bondline
Figure 5-6 shows the variation of shear and peel stresses along the bondline for different
overlap lengths. It can be observed that when the overlap length is equal to zero (Lo = 0 mm),
the peel and shear peak stresses are still important and the peel peak stress is even higher than
when no overply was added. For an overlap length equal to 5 mm, a drop in both shear and
peel peak stresses can be seen. However, since for this overlap length, the free edge of the
Experimental pristine value (N=4)
124
adhesive is not completely covered, a step is added in the bondline by the overply. This step
induces an additional peak in the shear and peel stress distributions at the beginning of the
bondline. This additional peak disappears with an overlap length of 10 mm, which covers the
entire free edge of the bondline, and an important drop in the shear and peel stresses along the
bondline is clearly visible.
Increasing the overlap length from 10 mm to 15 mm has little effect on the stresses distribution
along the adhesive bondline since the adhesive free edge was already entirely covered for
Lo = 10 mm. These results corroborate previously published results on the effect of overply on
peak stresses in scarf repair of solid composite laminates [22]. However, for monolithic
composite scarf repair [22], the critical overlap length was found equal to 5 mm instead of 10
mm in this study. This value depends in fact on different parameters and especially on the
adhesive thickness, the scarf angle and the ply thickness in the case of a stepped patch. To be
efficient, the overply should be long enough to cover entirely the free edge of the adhesive.
Referring to Figure 5-7, which represents the scarf-step repair configuration which is
considered in this study and the scarf-scarf configuration which is usually modelled in the
literature, a minimal value for the overply overlap can be determined using
sin tan
pao
ttL
in case of a scarf-step repair (36)
and
sin
ao
tL
in case of a scarf-scarf repair (37)
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The minimal overlap length in the case of a scarf-step configuration has obviously a larger
value than in the case of a scarf-scarf configuration. This means that a finite-element model
that simplifies the repair geometry using a scarf-scarf configuration will lead to an erroneous
value for the critical overlap length.
ii. Failure Load
Figure 5-8 shows the evolution of the failure stress in the facesheet as a function of the overply
overlap length. An increase in the strength is observed as the overlap length increases. It can
also be seen that a length of 10 mm can be considered as a critical value for this configuration.
From this overlap length, no major effect on the failure stress is observed. A much higher
strength recovery is obtained in comparison with the no overply configuration. This recovery
reaches about 90% of the pristine value. A change in the failure mode was observed too. While
the failure occurs in the adhesive bondline for the baseline configuration, failure occurs no
more in the adhesive but in the composite plies when an overply is added.
iii. Finite Element Model Validation
In order to validate the numerical predictions for the overply effect, tensile tests have been
conducted using the same methodology as presented in [76]. Three specimens with one (+45/-
45) overply and an overlap length of 10 mm were tested. The measured strength is indicated in
Figure 5-8. As can be seen, the strength has increased by 39 % compared to the one obtained
when no overply was used. However, the strength measured experimentally is slightly lower
than predicted. The results confirm nevertheless the important effect of the addition of an
overply on the strength recovery. Figure 5-9 shows the failure morphology of the tested
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specimens. It can be seen that failure occurs in the patch side and not in the scarf joint as it was
observed for the specimens with no overply [76].
a. Shear Stress distribution along the middle of the bondline.
b. Peel Stress distribution along the middle of the bondline.
Figure 5-6 Shear and peel stress distributions along the adhesive bondline as a function
overlap length Lo (3°-4-ply skin model).
127
Figure 5-7 Determination of the minimal overply overlap length
Figure 5-8 Repair strength prediction as function of the overlap length, Lo (3°-4-ply skin
model).
Figure 5-9 Failure morphology of a specimen with an overlap length, Lo=10.
tp
ta
tp
ta
(b) Scarf-scarf repair configuration
(a) Scarf-step repair configuration
Experimental pristine value (N=4)
10 m
m
Patch
Parent
128
Effect of Number of Skin Plies
The number of composite plies used for sandwich skins is usually much lower than for solid
composite laminates. It is therefore essential to investigate and understand how the skin
thickness may affect the residual strength of repaired sandwich structures. To study this effect,
repaired sandwich panels with 2-ply skins, 4-ply skins and 8-ply skins were modelled. The skin
lay-up sequence for each model is as follow:
- 2-ply skin: [(+45/-45)/ (0/90)]
- 4-ply skin: [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)]
- 8-ply skin: [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)/ (+45/-45)/ (0/90)/ (-45/+45)/ (90/0)]
To maintain a ply-by-ply match, change in number of plies was applied equally to the parent
part and the patch. Boundary conditions similar to the baseline configuration were applied.
i. Shear and peel stress distributions along the bondline
The shear and peel stresses along the adhesive bondline are plotted in Figure 5-10 for different
numbers of skin plies. The results are presented for the baseline scarf angle value of 3°. It can
be observed that as the number of plies increases, the peak stresses decrease near the bondline
ends. An important factor can explain these results: as the number of plies increases, the
number of (0/90) plies in the facesheet is increasing, so the proportion of the stress carried in
the outer-most (0/90) plies decreases. This results in lower peak stresses in the adhesive
bondline.
129
ii. Failure load
Figure 5-11 compares the failure stress obtained for the repaired sandwich panel with skins of
different thicknesses. It can be observed that the strength increases with the increase of the skin
thickness. One of the reasons is that when increasing the number of plies, the number of (0/90)
plies in the facesheet increases which reduces the peak stresses in the bondline. A higher
strength recovery is therefore obtained for the thicker facesheet. For the 2-ply and 4-ply skin
models, failure occurs in the adhesive bondline. However, for the thicker skin (8-ply skin),
failure occurs no more in the adhesive bondline but in the composite plies.
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a. Shear stress distribution along the middle of the bondline.
b. Peel stress distribution along the middle of the bondline.
Figure 5-10 Shear and peel stress distributions along the adhesive bondline as a function of
number of skin plies, N (α=3o).
131
Figure 5-11 Repair strength prediction as function of the number of skin plies, N (α=3°).
5.5 Discussion
Results of the parametric study show that peak stresses in the adhesive bondline are greatly
influenced by the scarf angle, the skin thickness and the overply overlap length. Therefore, the
strength of repaired sandwich panels will be very sensitive to theses parameters as well.
From the elastic-plastic analysis results, a map of the failure stress as a function of different
design parameters of the stepped-scarf joints was created. First, the number of skin plies (N)
was varied from two to eight, with scarf angles varying from 1.5° to 15°. Figure 5-12 shows
the evolution of the failure stress as a function of scarf angle for these numbers of plies. It can
be seen that, for a given scarf angle, the strength increases with the skin thickness. Therefore,
the higher failure stress is obtained here for an 8-ply skin sandwich. The failure mode has also
changed from failure in the adhesive bondline for N=2 and N=4 to composite failure for N=8
for scarf angles from 1.5° to 7°. For angles from 10° to 15°, the repair strength for N=8 is
Experimental pristine value
132
higher than for N=2 and N=4 but failure still occurs in the adhesive film. In the literature, a
scarf angle of 3o is often recommended for the design of scarf joints in composite structures. It
is true that for monolithic composite structures using this value allows designing high
efficiency repairs. For example, in the case of a repaired monolithic composite laminate with
a quasi-isotropic sequence ([02/452/-452/902]2s), Campilho et al. [20] obtained a full strength
recovery with a 3°-scarf angle. This angle is appropriate for monolithic composite laminates
because their lay-up counts usually at least eight plies. However, in the case of composite
sandwich structures, the skin is usually very thin and counts only a few plies. As observed in
Figure 5-12, using a 3o-scarf angle to repair a skin with four plies leads to strength recovery of
only 54%. Similarly, Ramantani et al. [52] used a 3o-scarf angle to repair a 4-ply sandwich
panel and obtained a 60% strength recovery. Therefore, due to their small skin thickness,
sandwich structures are more challenging to repair and require a lower scarf angle than
monolithic composite laminates.
The effect of adding an overply was also investigated for different skin thicknesses. Figure
5-13 presents the evolution of the failure stress as a function of the skin thickness for a repair
with no overply and a repair with a 10 mm-overlap length overply. The scarf angle was fixed
to 3°. The figure highlights the important effect of the addition of an overply for 2-ply and 4-
ply skin sandwiches. The strength becomes twice as important and failure occurs in the
composite plies. For the 8-ply skin sandwich, the increase in failure stress due to the overply is
less important since the strength was already high without an overply. The failure mode
remains the same (composite failure) as with no overply. Therefore, when repairing a thick
skin sandwich panel with a small scarf angle using an overply is not essential to obtain a good
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strength recovery. However, an overply is still useful to improve repair durability and protects
the tip of the scarf from being damaged.
It is confirmed from previous studies and this study that the failure stress of the repaired
composite sandwich panel increases as the scarf angle decreases. So, it is recommended to use
small scarf angle to insure a high strength recovery of the repaired sandwich structure. Large
scarf angles lead to smaller bond length, higher peak stresses in the adhesive and therefore
lower repair strength. On the other hand, smaller scarf angles requires removing a higher
quantity of composite material from the parent skin, which induces a larger repair area in the
structure. From this study, we highlight the importance of the addition of an overply to restitute
the strength of the repaired structure. Therefore, an alternative to using a very small scarf angle
to restore the structure strength is to add an overply with an overlap length that covers entirely
the free edge of the adhesive. This will allow designing an efficient repair using a more
reasonable scarf angle that does not require removing a great quantity of undamaged material.
For very thin facesheet, however, it is recommended to use a very small scarf angle and an
overply to obtain a high strength restitution.
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Figure 5-12 Map of the failure stress as a function of the scarf angle and number of plies,
N.
Figure 5-13 Variation of the failure stress as a function of the overply and number of skin
plies, N (α=3°).
Failure in the adhesive film
Failure in the composite plies
Experimental pristine value (N=4)
Experimental pristine value
135
5.6 Conclusions
The effect of geometrical design parameters (scarf angle, overply overlap length, number of
skin plies) on the shear and peel stress distributions in the adhesive bondline and on the failure
stress of a stepped-scarf repair of composite sandwich structures have been thoroughly
investigated. Two material models were used for the adhesive film: a linear elastic and a non-
linear elastoplastic model with shear failure criterion. A failure criterion based on maximum
fiber strain was used to predict failure of the composite skins. It has been shown, by both
numerical analyses and experiments, that the geometrical design parameters can influence
greatly stresses distributions along the bondline and the repair strength.
Stresses distribution along the adhesive bondline
Results showed that the shear and peel peak stresses are very sensitive to scarf angle, the
addition of an overply and the number of skin plies. It was shown that the adhesive peel and
shear stresses vary greatly along the adhesive bondline as a function of the ply orientation with
the (0/90) plies inducing the most critical stress peaks. As the number of plies in the skin
increases, the load is transferred through more (0/90) plies and the stress peaks decrease. With
the addition of an overply with an overlap length that covers entirely the free edges of the
adhesive, a considerable decrease of the peak stresses is observed. Hence, it can be concluded
that the addition of an overply can provide a good protection to the adhesive joint and reduce
the peak stresses that may cause premature failure of the repaired structure.
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Failure stress prediction
Two possible types of failure were taken into account in order to predict the residual strength
of the repaired sandwich panels with the different design parameters: failure in the adhesive
bondline and failure in the composite plies.
It was observed that failure occurs in the adhesive film for angles from 1.5° to 15°. The highest
strength is obtained for the 1.5° scarf angle and reaches 62.7 % of the pristine panel strength.
With the addition of an overply the strength recovery increases to about 90% for a 3°-scarf
angle. Failure occurs mainly in the composite skins and no more in the adhesive film where the
stress peaks are reduced because of the overply.
With the increase of the number of skin plies, failure stress of the repaired composite sandwich
panel increases. For the 2-ply and 4-ply skin models, failure occurs in the adhesive bondline.
However, for the thicker 8-ply skin, failure occurs no more in the adhesive bondline but in the
composite plies.
Correlation between experimental and finite-element results
Experimental results were used to validate the numerical predictions in terms of failure stress
and failure path. Comparison with the experimental results confirmed that the developed model
provides a good prediction of the repaired joint strength and failure mode and it may be used
as an alternative design tool to study the mechanical behavior of repaired composite sandwich
panel.
137
From this study, we highlight the considerable effect of the skin thickness and the addition of
an overply on the residual strength of repaired sandwich structures. Due to their small
thickness, sandwich skins are much more critical to repair than solid composite laminates. It is
crucial in the design of efficient repair for sandwich structures to use smaller scarf angles than
for solid composite laminates and to use an overply.
Acknowledgements
We would like to thank the Natural Sciences and Engineering Research Council of Canada
(NSERC), the Consortium for Research and Innovation in Aerospace in Quebec (CRIAQ), the
National Research Council Canada (NRC), Bombardier Aerospace and L3-MAS for funding,
technical support and materials.
138
Chapter 6.
Article 3: Evaluation of the mechanical
performance of repaired composite sandwich
structure using different mechanical tests
Emna Ghazali, Marie-Laure Dano, Augustin Gakwaya and Charles-Olivier Amyot
Résumé
Cet article décrit les performances mécaniques de réparations collées sur des panneaux
sandwich fabriqués avec des peaux en de carbone-époxy et une âme Nomex. Tout d'abord, le
comportement mécanique des panneaux sandwich intacts et réparés sous chargement de
compression et de flexion en quatre points a été étudié. Ensuite, des analyses bidimensionnelles
(2D) par éléments finis sont effectuées pour prédire la résistance à la rupture des réparations
sous chargement de flexion quatre points. Un comportement élastoplastique avec un critère de
rupture en cisaillement a été considéré pour le film adhésif. L’âme en nid d'abeilles est
modélisée par un matériau élastique orthotrope linéaire équivalent et les peaux composites sont
considérées comme un matériau linéaire orthotrope avec un critère de contraintes maximales
pour déterminer la rupture du premier pli. Les résultats expérimentaux obtenus à partir des
essais de flexion quatre points et de compression sont similaires à la fois pour les panneaux
sandwich intacts et réparés.
139
Abstract
This paper studies the static mechanical performance of adhesively bonded repairs on sandwich
panels made with carbon-epoxy composite skins and a Nomex core. First, the mechanical
behavior of pristine and repaired sandwich panels under edgewise compressive, tensile and
four-point bending loadings is studied experimentally. Then two-dimensional (2D) finite
element analyses are performed to predict the repair strength under the different load cases.
The adhesive film behavior is described using an elastic-plastic model with a shear failure
criterion while the honeycomb core is assumed to respond like an equivalent orthotropic linear
elastic material and the composite skins are considered as an orthotropic linear material with a
maximum strain criterion used to determine the fiber failure load. Results from the tensile and
four-point bend tests are comparable for both pristine and repaired sandwich specimens.
However, edgewise compression and four-point bend tests have not provided equivalent
results. The study concludes that flexure tests are preferred over tensile and edgewise
compressive tests. It provides a reliable and simple test method to determine the mechanical
behavior of repaired sandwich panels.
Keywords: sandwich, repair, compression, tension, flexure tests, 2D finite element analysis
6.1 Introduction
Composite sandwich structures are increasingly being used for primary aircraft components
because of their superior structural performance such as high strength, high stiffness, long
fatigue life, and light weightiness [43]. Although composite structures offer many other
advantages over traditional metallic structures such as better fatigue resistance and being less
140
prone to deterioration caused by corrosion and cracking, they are more sensitive to other type
of damage such as impact damage that may cause delamination, disbonding and internal
material crushing. As these damages can cause severe reduction in strength and stiffness and
may lead to the structure failure, it is crucial to have effective repair methods capable of
restoring the structural performance of damaged composite structures. In the literature, two
major repair configurations have been investigated: bolted and bonded repair patches [77, 78].
Bonded patch joining (scarf, step, overlap) are often used when high strength recovery and
aerodynamic requirements need to be satisfied [79]. The mechanical performance of repaired
composite structures is usually assessed by experimental testing. For that, robust and reliable
methods need to be provided.
To study the mechanical performance of repaired honeycomb sandwich structures, several
experimental studies have been carried out under different static loads. The studied repairs were
either across the width of the specimen [47] or circular [49]. Edgewise compressive tests are
the most common test methods that have been used in the literature. To perform such test
methods, a CAI fixture system is widely used. The included anti-buckling guides may help to
prevent buckling failure from occurring during the test. However, ends-failure crushing cannot
easily be prevented from occurring, especially for pristine sandwich panels.
The AGARD (Advisory Group for Aerospace Research & Development) [44] published a
report on repairs of sandwich structures used in military structures. The sandwich structure was
repaired using external patches. The patches were either co-cured or pre-cured and the core
either replaced or filled with a filler paste cured at high and low temperatures cycles. Static and
fatigue edgewise compressive tests were carried out to characterize the behavior of the repairs.
141
Results showed that the pre-cured patch method is the most suitable for field-level application.
Liu et al. [49] investigated the mechanical performance of circular repaired sandwich panels
using the edgewise compressive tests, at room temperature conditions. Recently, Zhang et al.
[50] published a study on the mechanical performance of honeycomb sandwich panels with
open-hole damage and circular scarf repair under compressive loads. A good agreement was
found in terms of ultimate failure load and damage shape between the experimental and
numerical results. Failure of the repaired sandwich panel was due to adhesive delamination and
patch local buckling.
Strength of repaired honeycomb sandwich panels has also been assessed in the literature using
four-point bending. Baker et al. [45] have studied experimentally a scarf repair on a horizontal
stabilizer of an F/A-18 spacecraft composed by an aluminum honeycomb core and CFRP skins.
The repaired structure was tested under a four-point bending load. The specimens were tested
at -40ºC, room temperature and 104ºC, in dry and wet conditions. The failure of the adhesive
film was cohesive for all test conditions. At 104ºC, the failure strains were reduced by 50%,
compared to the ones of the specimens tested at room temperature. Mahdi et al. [47] have
studied the performance of both pristine and scarf repaired sandwich panels subjected to static
four-point bending loads. The repaired facesheets were loaded in both compression and tension.
Two repair configurations were studied: overlap and scarf repair. The repair was cured at low
and high temperature systems. The main findings of this work are that when loaded in
compression, the scarf repairs were weaker than overlap repairs. However, scarf repairs were
stronger in tension achieving 100% of the pristine strength. To perform such tests, long beams
were manufactured by the authors and a large fixture system was used.
142
A series of experimental tests (tensile, shear and four-point bend tests) were conducted by
Tomblin et al. [2] to study the effects of different process parameters on the quality of 2D
sandwich panel scarf repairs. Most of the repaired specimens tested under different loads
showed a high strength recovery (about 92%). As a conclusion of their work, a methodology
for the repair process along with design tools for damage tolerance on sandwich structures were
developed.
Currently, no comparison study of the effect of each test method to assess the mechanical
performance of repaired honeycomb sandwich panels has been conducted in the literature. This
paper investigates the assessment of the mechanical performance of both pristine and repaired
panels using three different mechanical tests: tensile, edgewise compressive and four-point
bend tests. It focuses on one aspect of a larger research program on the repair of sandwich
structures [80]. Its objective is to compare the performance of different test methods used to
assess the mechanical behavior of repaired honeycomb sandwich panels. Both experiments and
finite element analyses are performed. Firstly, the repair procedure and the experimental set-
up are detailed. Force or stress versus strain curves are presented for the different experimental
tests and a series of fractography images are shown to determine the failure mode and pattern
of the repaired sandwich panels. Secondly, the finite element models developed using the
commercial software ABAQUS [56] are discussed. The obtained numerical results are
compared with experimental results to validate the finite element model predictions of the
failure load of the repaired sandwich panel under different loadings.
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6.2 Experimental Work
6.2.1 Materials
The composite honeycomb sandwich panels were composed of four-ply woven Carbon Fiber
Reinforced Polymers (CFRP) skins bonded to an over-expanded or a hexagonal Nomex
honeycomb cores with a 19 mm and 25.4 mm thickness, respectively. The skin material was a
plain weave out-of-autoclave (OOA) semi-impregnated prepreg (CYCOM 5320 T650 PW
from Cytec Engineering Materials). The laminate used for the two skins had a [(+45/-45)/
(0/90)/ (-45/+45)/ (90/0)] quasi-isotropic stacking sequence. The Cytec FM® 300-2M adhesive
film used to bond the skins to core is a toughened epoxy B-staged adhesive film. This adhesive
film is common for repair and had a nominal thickness of 0.25 mm. The presence of polyester
fibers non-woven carrier, which accounts for 5–10 wt. %, ensures constant bondline thickness.
The over-expanded Nomex core is a phenolic resin impregnated aramid honeycomb core (Euro
Composites ECA-R 4.8 64), with a cell size of 4.8 mm and a density of 64 kg/m3. The
hexagonal Nomex core was a phenolic resin impregnated aramid honeycomb (Euro
Composites ECA 3.2 96), with a cell size of 3.2 mm and a density of 96 kg/m3.
6.2.2 Repair Procedure
The mechanical behavior of sandwich panels repaired using a stepped-scarf bonded joint
configuration was studied. The actual repair was carried out on the tool facesheet (TF). To
create the scarf in the parent facesheet, each prepreg ply had an initial rectangular cut-out as
shown in Figure 6-1. The cut-outs had a specific width such that when stacked together the
144
plies formed a drop-off. The FM300-2M adhesive film was used to bond the two facesheets to
the core. Then, both skins and core were co-cured under vacuum bag in an oven.
The repair patch was manufactured as follows. After cure of the parent part, the step shaped
parent area was sanded by a 120-abrasive paper to reach the desired scarf angle. This was
followed by a surface clean up with acetone and completed immediately by drying. The repair
patch was prepared using the same parent prepreg material and the original stacking sequence.
The plies were cut to a specific width and stacked together to form an overlap as shown in
Figure 6-2. The overlap distance Loverlap was determined from the scarf angle α and the ply
thickness tp using:
tan
p
overlap
tL
(38)
6.2.3 Specimen Preparation and Test Procedure
As a next step, static mechanical tests were performed to compare the performance of the
repaired panels with that of the pristine. The sandwich specimens were tested under
compressive, tensile and four-point bending loadings. Table 6-1 summarizes the test matrix
followed for each load configuration. As seen, repairs with three different scarf angles were
tested in tension and compression whereas only 3o-scarf angle repairs were tested in flexure.
Table 6-1 Test matrix for different experimental tests
Configuration Angle (°) Tension Compression Flexion
Pristine - 3 4 3
Repair
3 3 3 2 (TF in tension)
3 (TF in compression)
5 3 3 -
7 3 3 -
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Figure 6-1 Parent panel dimension (not to scale)
Figure 6-2 2D stepped-scarf repair configuration
Edgewise Compressive Tests
The pristine and repaired sandwich panels were cut into rectangular test specimens using water
jet at a nominal size of 305 mm by 102 mm. To prevent end-failure, special considerations in
the panel preparation were made. A section of the core material was removed at the top and at
the bottom of the specimen and replaced with a high stiffness potting material to reinforce the
edges. This section was 13 mm high and 102 mm wide. Aluminum tabs were then bonded at
both ends to ensure a smooth load transfer in the potting-Nomex core junction, as seen in Figure
6-3.
α
α
146
A fixture system similar to the one recommended by the ASTM standard D7137 [81] for
compression after impact (CAI) test was used to hold the specimens and to introduce
compressive loading, as shown in Figure 6-4. Specimens were tested at a crosshead
displacement rate of 0.5 mm/min, according to ASTM standard C364 [82], in an
electromechanical MTS machine with a 100 kN load cell. Three strain gages were bonded on
the specimens to make sure that there is no bending due to specimen misalignment and to study
the strain distribution on the skins. Gage 1 was bonded in the middle of the tool face (Figure
6-5.a) and the two others, gages 2 and 3, on the bag face, as depicted in Figure 6-5.b. The tool
face surface of the specimen was also prepared for measurement with a 3D digital image
correlation (DIC) system (Aramis by Gom [73]). The DIC software was then used to determine
the full in-plane and out-of-plane displacements and strain field on the specimen tool face
surface during testing. The applied load and the strain response were recorded during the test.
The quality of the repair was assessed by microscopic observation before testing (see
micrograph of Figure 6-6). No micro-cracks or damaged cells were observed in the repair area.
Moreover, no porosity was visible along the repair bondline. However, macro porosity was
observed in the adhesive between the core and the skins.
147
Figure 6-3 Specimen geometry (not to scale)
Figure 6-4 CAI fixture system used for the edgewise compressive tests
a. Pristine sandwich panel b. Repaired sandwich panel
Aluminum tabs
148
Figure 6-5 Location of strain gages (not to scale)
Figure 6-6 Micrograph of the repair cross-section before testing
Uniaxial Tensile Tests
Rectangular pristine and repaired test specimens were cut with a water jet-milling machine at
a nominal size of 335 mm by 102 mm to be tested under uniaxial tensile loading. To prevent
ends failure, the specimen ends were reinforced with aluminum inserts and aluminum tabs.
Specimens were tested with the same 100 kN electromechanical testing machine, at a constant
crosshead rate of 1 mm/min. A homemade tensile test fixture, inspired from the one used by
Tomblin et al. [2], as shown in Figure 6-7, was used for these tests. The surface of the tool
facesheet was prepared for measurement with a 3D digital image correlation (DIC) system
(Aramis by Gom [73]). A video extensometer was used to measure the strain on the bag
a. Tool face (TF) b. Bag face (BF)
Patch
Porosity
Parent
149
facesheet. The strain field measured by the DIC system was averaged on an area taken in the
middle of the specimen to obtain a single value that can be compared to the strain measured by
the video extensometer. For the repaired specimens, the strain was averaged in the middle of
the patch.
Figure 6-7 Tensile test set-up.
Four-Point Bend Tests
Long sandwich beams were used for the pristine configuration (686 x 76.2 mm2) in comparison
to the 3°-repaired beams (610 x 76.2 mm2). The length had to be increased to prevent core
shear and core crushing failure modes from occurring. Specimens were tested using the same
100kN electromechanical testing machine at a crosshead rate of 8 mm/min. A fixture system
similar to the one used in the ASTM standard D7249 [83] was machined, as illustrated in Figure
6-8. Four 3 mm-thick rubber pads were used under the loading points to prevent core crushing.
The loading points were placed at different distances for the pristine and repaired sandwich
150
beams respectively, as seen in Figure 6-8.b and Figure 6-8.c. Strains gages and a DIC system
were used to measure the strains on the specimens. First, the repaired beams were placed in the
fixture with the repair on the top so that compressive load was applied on the repaired skin.
Then, they were placed in the fixture with the repair on the bottom so that tensile load was
applied to the repaired skin.
Figure 6-8 Four-point bend test fixture and specimen configurations (not to scale)
L
S
a. Four-point bending fixture
c. Repaired sandwich beam
b. Pristine sandwich beam
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6.2.4 Results and Discussion
Edgewise Compressive Tests
The compressive test results are presented in Figure 6-12 to Figure 12. The load versus strain
curves obtained for the pristine and for the 3°-repaired specimens are shown in Figure 6-9. It
can be observed that the behavior of the tested specimens remains linear until failure occurs
suddenly. Similar results were observed for the specimens repaired using 5°- and 7°- scarf
angles. Several curves representing the force versus strain measured using different instruments
are shown in Figure 6-10. It can be observed that the strains measured on the bag facesheet
(gages 2 and 3) are slightly different from the strains measured on the tool facesheet (gage 1
and DIC). This difference was noticed for all tested specimens (pristine and repaired). This
may be due to the presence of a slight bending in the tested specimens.
Different failure modes were observed for the pristine and for the repaired sandwich panels.
For the pristine panels, failure occurred near the loaded edges which may be caused by a lack
of uniformity of the load distribution in the specimen. The repaired specimens failed away from
the loaded ends by local buckling in the scarf area, as clearly shown with the DIC measurement
presented in Figure 6-11. An out-of-plane displacement was observed and measured by the
DIC system. To determine the appropriate failure modes and pattern induced in the tested
repaired specimens, fractography was performed using optical microscopy. Figure 6-12 shows
the resulting micrographic images. From that figure, cracks can easily be observed in the parent
laminate, a few core cells are fractured, and no damage was noticed in the patch or in the
adhesive. Failure seems to be due to skin wrinkling as shown in Figure 6-11. Severe
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discontinuity in the structure stiffness may be responsible for the observed failure mode.
Results obtained for the tested specimens are summarized in Table 6-2. The strength was
evaluated from the applied load by:
2
f
f
P
t w (39)
where tf is the facesheet thickness, w is the specimen width and P is the failure compressive
load.
A reduction in residual compressive strength for the repaired panels was observed. Only 53 %
of the strength was recovered for the 3°-repaired panels. It can be noticed also that the strength
increases slightly with the increase of the scarf angle and it reaches about 67.5% for the 7°-
repaired panels. These results may be explained by the type of failure mode encountered (local
buckling of the repaired facesheet). As the scarf angle increases, the scarf length decreases, and
the discontinuity area is reduced.
Figure 6-9 Typical force versus strain curves for pristine and 3°-repaired sandwich
specimens tested in compression
153
Figure 6-10 Force-strain curves obtained using different strain measuring instruments for
pristine and 3°-repaired sandwich specimens tested in compression
Figure 6-11 DIC measurement: out-of-plane displacement of 3°-repaired sandwich
specimen tested in compression at failure
[mm]
Patch
repair
Parent
Parent
a. Pristine sandwich specimens
b. 3°-repaired sandwich
specimens
154
Figure 6-12 Micrograph of the repair cross-section after failure of 3°-repaired sandwich
specimen tested in compression
Table 6-2 Summary of the compressive test results
Configuration Angle
(°)
Failure strength
(MPa)
Strength recovery
(%)
Pristine - 74.40 -
Repair
3 198.02 52.89
5 228.06 60.91
7 252.53 67.45
Uniaxial Tensile Tests
The results of the static tensile tests performed on the pristine and the 3°-repaired sandwich
specimens are presented in Figure 6-13. The graphics represent the load versus strain measured
on the tool facesheet with the DIC system. As can be observed, the load-strain behavior is
mostly linear until failure for both the pristine and the 3°-repaired specimens. For the 5°- and
7°-repaired specimens, a similar trend for the load-strain curves was also observed. A summary
of the tensile test results for the different configurations is shown in Table 6-3. The failure
stress is calculated using equation (2) as for the compressive tests. For the pristine panels,
Crack/porosity
Parent laminate
Damaged cell
Crack
Parent laminate
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damage occurred in both facesheets far from the loaded ends. For the repaired panels, failure
occurred mainly in one of the two scarf zones for the different studied scarf angles.
Four-Point Bend Tests
The stress in the sandwich beam skins tested under four-point bending is calculated using:
( )
2( )
f
f
P S L
d c bt
(40)
where P is the applied force, S is the support span, L is the load span, c is the core thickness, d
is the measured total thickness of the sandwich panel, b is the width of the specimen and tf is
the facesheet thickness.
Figure 6-14 shows the flexure stress-strain responses for the pristine and for the 3°-repaired
sandwich beams with the repaired facesheet loaded in compression or in tension. The stress-
strain curve for the pristine beam is very smooth because the strains were measured using strain
gages. The observed non-smoothness in the stress-strains curves of the 3°-repaired beams is
due to noise induced in the strain measurement with the DIC system. The obtained
experimental curves indicate that the flexure response is linear until failure suddenly occurs.
For the pristine beams, failure occurs in the facesheet loaded in compression. However, for the
3°-repaired sandwich beams loaded in tension, failure occurs along one of the double scarf, as
illustrated in Figure 6-15. The same failure mode is observed when the 3°-repaired sandwich
beam is loaded in compression, i.e. the failure occurred in one of the double scarf. A summary
of the flexure test results for the different studied configurations is shown in Table 6-4.
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It can be noted that when the repair is loaded under four-point bending with the repaired face
in compression, a strength recovery of 55.16 % is obtained. However, a higher recovery of
63.68% is obtained when the repaired face is loaded in tension. These results show that the
repaired beams are more efficient when loaded in tension than in compression.
Figure 6-13 Typical axial load-strain curves for the pristine and 3°-repaired sandwich
specimens tested under tension
Table 6-3 Summary of the tensile test results
Configuration Angle
(°)
Failure strength
(MPa)
Strength recovery
(%)
Pristine - 537 -
Repair
3 276 51.39
5 272.54 50.75
7 271 50.46
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Figure 6-14 Typical stress versus strain curves for pristine and 3°-repaired sandwich beams
tested under four-point bending
Figure 6-15 . Failure mode of a 3°-repaired sandwich beam tested under four-point bending
(repair in tension)
Table 6-4 Summary of the flexure test results
Configuration Angle
(°)
Failure strength
(MPa)
Strength recovery
(%)
Pristine - 420.60 -
Repair in compression 3 232.02 55.16
Repair in tension 3 267.85 63.68
Parent Patch
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Comparison and Discussion
The main objective of the flexure tests conducted on the composite sandwich beams was to
validate the results obtained for the pristine and for the repaired panels tested under edgewise
compressive and uniaxial tensile loads.
Figure 16 shows the failure stress obtained for static edgewise compressive, uniaxial tension
and four-point bend tests for the pristine specimens. As seen in Figure 6-16, pristine sandwich
specimens exhibit a higher strength in tension than in compression. This explains why, when
tested in flexure, failure occurs on the compressive side of the pristine sandwich beam. A higher
strength was obtained from the four-point bend tests in comparison with the edgewise
compressive tests. These results are explained by the difference in the failure mode. Pristine
specimens failed at the CAI fixture loading points in the free-length between the contact surface
and the anti-buckling support, when loaded under edgewise compressive load. This makes it
difficult to obtain a valid pristine compressive strength. However, pristine beams tested under
four-point bending failed on the compressive side within the load span away from the loading
points.
Figure 6-17 presents the failure stress for the pristine and the 3°-repaired specimens tested
under flexure loading with the repair face loaded in compression and in tension with those
obtained under uniaxial compression and tension loads. Here, the failure stress obtained in the
case of uniaxial tension and four-point bending (with the repair in tension) is quite similar.
Both test methods revealed the same failure mode for the 3°-repaired specimens, i.e. an
adhesive failure in one of the double scarf.
159
The 3°-repaired specimens tested under four-point bending (with the repair in compression)
reached a higher failure stress in comparison with the 3°-repaired specimens tested under
edgewise compressive load. A local facesheet buckling mode, a facesheet wrinkling (as
depicted in Figure 6-11) was detected for the repaired specimen under edgewise compression
and may explain this difference in the stress value.
From the different tests results, the four-point bend test was found to be less sensible to loading
issues caused by the fixture system in comparison with the edgewise compression tests.
Compressive tests were found to be susceptible to the test fixture and ends-crushing failure,
especially for the pristine panels. Tensile tests provided reliable results. However, they were
very expensive in terms of time and resources to be performed (cost of test fixtures and
specimen preparation). The Digital Image Correlation system, however, could easily be used
with the uniaxial loading tests since the specimen surface was clearly visible. Difficulties using
DIC were encountered with the flexure tests since the fixture does not allow a direct access to
the specimen surface. Mirrors can be used but may cause strain measurement variation.
Another drawback of the flexure tests is the need for large beams to avoid premature failure
modes such as core crushing or core shear and therefore large test fixtures are required.
Despite the mentioned disadvantages, four-point bend tests can assess correctly the mechanical
behavior of pristine and repaired sandwich panels and offer the facility of specimen
preparation. As such, four-point bend test is suitable and simple as test method for evaluation
of the mechanical performance of repaired sandwich panels.
160
Figure 6-16 Comparison of the failure stress of the pristine panels obtained from different
loading types.
Figure 6-17 Comparison of the failure stress of the 3°-repaired panels obtained from
different loading types.
161
6.3 Finite Element Analysis
In this section, numerical simulation of the carried-out experiments was performed in order to
evaluate the ability of a previously developed finite element model to capture the
experimentally observed behavior of the repaired sandwich specimens. The finite element
model has been developed and validated using tensile tests in previous work [76].
6.3.1 Model Description
The analysis takes into account von Mises plasticity with a shear failure criterion for the
adhesive film [76] to predict the mechanical behavior of the bonded joints until failure. Because
a rectangular repair patch across the panel width was studied, a plane strain assumption was
adopted in the finite element modeling process to study the mechanical behavior of the adhesive
joint as a two-dimensional (2D) problem. Hence, a longitudinal cross-section corresponding to
the middle of the panel away from the edge in the width direction was modeled. Since the
repaired beam was symmetric with respect to its midsection, one can exploit this symmetry
condition and model only half of the repaired panel, as illustrated in Figure 6-18. The
mechanical properties of the CFRP woven composites, the two honeycomb cores and the
adhesive film are listed in Table 6-5, Table 6-6, Table 6-7and Table 6-8, respectively.
The finite element (FE) models were developed using the commercial software ABAQUS [56].
Two-dimensional quadrilateral plane strain solid elements with reduced integration CPE4R,
from Abaqus element library [56], were used to model the two skins, the honeycomb core and
the adhesive film. For the edgewise compressive and uniaxial tensile tests, a displacement as
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measured from the experiment was applied at the left edge (x=L) and symmetric conditions
were imposed on the right edge (x=0).
For the four-point bend model, the section between the two loading points was subjected to a
constant moment. This moment was applied at a reference point. The element nodes were
linked to the reference point using TIE constraints. The boundary conditions are defined as
follow. The left edge (x=L) was subjected to a moment, determined from the ultimate force
applied experimentally, by a kinematic coupling constraint point (reference point), as described
in Figure 6-19. On the right edge (x=0), symmetric boundary conditions were imposed.
Each single woven ply and the adhesive film were discretized through the thickness using two
and four elements respectively, as illustrated in Figure 6-20. The adhesive film along the joint
as well as between the two skins and the core was modelled too. The Nomex honeycomb core
was discretized through the thickness using five elements.
Figure 6-18 Studied longitudinal cross-section of the repaired specimens
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Figure 6-19 Model geometry and boundary conditions for the four-point bend test
Figure 6-20 Mesh details of the adhesive bondline
Table 6-5 Elastic material properties of the plain weave carbon-epoxy ply
E1 (GPa)
E2 (GPa)
E3 (GPa)
64.6a
64.6a
10b
G12 (GPa)
G13 (GPa)
G23 (GPa)
4.9a
4.9b
4.9b
ν12
ν13
ν23
0.047a
0.3b
0.3b
a experimentally measured
b assumed
Table 6-6 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R
4.8 64)
EW (MPa)
EL (MPa)
ET (MPa)
30.3a
0.089a
185a
GWL (MPa)
GWT (MPa)
GLT (MPa)
1.9b
55.5c
21.1c
νWL
νWT
νLT
0.26b
0.22b
0.022b
a experimentally measured
b estimated from [64]
c from manufacturer
RP
Symmetric
conditions M
X=0 X=L
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Table 6-7 Mechanical properties of the hexagonal Nomex honeycomb core (ECA 3.2 96)
EW (MPa)
EL (MPa)
ET (MPa)
19.2
25.6
379.2
GWL (MPa)
GWT (MPa)
GLT (MPa)
5.13
68a
96a
νWL
νWT
νLT
0.85
0.020
0.027
a from manufacturer. The other values are estimated based on [64]
Table 6-8 Mechanical properties of the FM300-2M adhesive film
E (GPa) ν12 τy (MPa)
2.024 0.3 30
6.3.2 Model Results
The model was used to predict the mechanical behavior of the 3°-repaired sandwich panels
until failure for the tensile, compression and flexure tests. Figure 6-21 compares the predicted
and experimental measured strength values. The failure stress was well predicted for the 3°-
repaired sandwich panels under tensile and four-point bending loads. For the 3°-repaired
sandwich panels under edgewise compressive loads, the FE model overestimates the strength.
This is because the experimentally obtained failure is due to face wrinkling and this failure
mode is not considered in the developed FE model. An error inferior to 15% was found for the
different load cases. This error value was calculated using:
(%) 100FE Exp
x x
Exp
x
Error
(41)
The deformed shape of the repaired sandwich beam predicted by the FE model is presented in
Figure 6-22 when loaded under four-point bending with the repair on the compressive side. As
can be seen, failure occurs mainly in the adhesive bondline and propagates in the adhesive
between the core and the facesheet. When loaded under four-point bending with the repair in
tension, a similar failure morphology was obtained. This failure mode is in accordance with
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the failure observed experimentally. These results, in term of strength and failure mode
predictions, validate the use of the developed finite element model for predicting the
mechanical behavior of the repaired sandwich panels under four-point bending and uniaxial
tensile loads. However, for the compressive tests, as the face wrinkling failure mode is not
taken into account in the model, the strength is not well predicted. An improvement of the FE
model is needed to well predict the behavior of repaired panels under edgewise compressive
loads.
Figure 6-21 Numerical predictions versus experimental results for 3°-repaired sandwich
specimens under different load cases.
166
Figure 6-22 Deformation and failure mode for a 3°-repaired beam tested under four-point
bending (repair in compression)
6.4 Conclusion
Bonded repair has been conducted on composite sandwich panels and several mechanical tests
were carried out to evaluate their strength. Pristine and repaired specimens were tested under
four-point bending with the repair loaded in compression and in tension, under uniaxial tension
and edgewise compression. The influence of the experimental test used to determine the
performance of pristine and stepped-scarf repaired composite sandwich structures has been
thoroughly investigated. The main results are:
Strength recovery and failure mode
A low strength recovery was observed for the repaired sandwich panels. This may be explained
by the fact that failure mainly occurs in the adhesive. The use of an overply would have
probably decreased the stress in the adhesive joint and increased the repair strength.
Experimental mechanical tests
Parent Patch
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Different experimental tests were used to determine the mechanical performance of pristine
and repaired composite sandwich panels. Results showed that failure stress and failure mode
are similar for repairs loaded in tension through uniaxial tensile tests or four-point bend tests.
However, edgewise compression and four-point bend tests do not provide equivalent results.
The strength obtained through four-point bending is higher for both the pristine and the repaired
panels.
Each experimental method has its advantages and drawbacks. Both tensile and compressive
tests were expensive in terms of fixture systems and specimen preparation, but they offer the
possibility of using DIC that facilitates the detection of failure modes. Flexure tests provide
similar results as the tensile tests but have the advantage of being faster and easier to perform
since no specimen preparation is required. However, long sandwich beams and a large fixture
system need to be manufactured in order to prevent the occurrence of premature failure such
as core shear or crushing, depending on the core and skin material properties.
Correlation between experimental and numerical finite element results:
Experimental results were used to validate the numerical predictions in terms of failure stress
and failure mode. Comparison of numerical results with the experimental results confirmed
that the developed model provides a good prediction of the repaired joint strength and failure
mode and hence may be used as an alternative design tool to study the mechanical behavior of
repaired composite sandwich panel.
The objective of this study was to evaluate the use of experimental test methods to determine
the mechanical performance of repaired honeycomb sandwich panels. From the results, it can
168
be concluded that flexure tests are preferred over tensile and edgewise compressive tests. It
provides a reliable and simple test method to determine the mechanical behavior of repaired
sandwich panels.
ACKNOWLEDGEMENT
We would like to thank the Natural Sciences and Engineering Research Council of Canada
(NSERC), the Consortium for Research and Innovation in Aerospace in Quebec (CRIAQ), the
National Research Council Canada (NRC), Bombardier Aerospace and L3-MAS for funding,
technical support and materials
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Chapter 7.
Article 4: Experimental and Numerical Studies of
Stepped-Scarf Circular Repair in Composite
Sandwich Panels
Emna Ghazali, Marie-Laure Dano, Augustin Gakwaya and Charles-Olivier Amyot
Résumé
Cet article étudie la performance mécanique des réparations circulaires collées sur des
panneaux sandwich fabriqués avec des peaux composées de carbone-époxy et une âme en
Nomex. Tout d'abord, le comportement mécanique des panneaux sandwich intacts,
endommagés et réparés sous chargement de compression est étudié. Ensuite, des poutres
sandwich intactes et réparées sont testées sous un chargement de flexion quatre points où la
réparation circulaire est chargée en tension. Enfin, des analyses par éléments finis sont
effectuées pour prédire la résistance à la rupture des structures sandwich réparées. Le film
adhésif a été considéré comme un matériau élastoplastique avec un critère de rupture en
cisaillement. L’âme en nid d'abeille se comporte comme un matériau élastique linéaire tandis
que pour les peaux composites, un modèle d’endommagement progressif pour les composites
tissés est utilisé pour prédire le comportement de la peau jusqu'à la rupture. La corrélation entre
la rigidité et la résistance obtenues à la fois par les mesures expérimentales et les prédictions
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par éléments finis, pour les structures étudiées, indique que le modèle par éléments finis
développé est un outil d'analyse efficace pour la prédiction du comportement mécanique des
panneaux réparés.
Abstract
This paper investigates the static mechanical performance of bonded circular repairs on
sandwich panels made with carbon-epoxy composite skins and a Nomex core. First, the
mechanical behavior of pristine, open-hole and repaired sandwich panels under edgewise
compressive loading is studied. Next, pristine and repaired sandwich beams are tested under
four-point bending with the circular repair loaded in tension. Then, finite element analyses are
performed to predict the strength of the repaired sandwich panel. The adhesive film was
considered as an elastic-plastic material with a shear failure criterion. The honeycomb core is
assumed to behave as a linear elastic material while for the composite skins, a progressive
damage model for woven fabric composites is used to predict the skin behavior until rupture.
The good agreement between stiffness and strength levels obtained from both experimental
measurements and finite element predictions, for pristine, open-hole and repaired sandwich
panels, indicates that an effective analysis tool for the mechanical behavior of the repaired
panels has been set-up.
Keywords: composite sandwich structures, adhesively bonded repair, finite element analysis,
progressive damage
171
7.1 Introduction
Since fiber-reinforced composite structures offer superior strength, higher stiffness, lighter
weight and greater durability [43], they are increasingly being used for primary aircraft
components traditionally made of metallic materials. However, despite their good properties,
composite airframe structures are more sensitive to impact damage which can cause
disbonding, delamination and internal crushing. Considering their extended service life and
operating conditions, the extent of damage determines whether the composite components need
to be repaired or replaced. Hence, to take full advantage of their many benefits, it is necessary
to ensure that these structures are durable, repairable, and maintainable. Since fiber-reinforced
composite sandwich structures are increasingly being used in aircraft components, it has
become necessary to develop effective repair methods that will restore the component’s
original design strength.
Several studies have been conducted on bonded scarf and stepped joint repairs of monolithic
composites laminates. Campilho et al. [17, 20, 34, 71-72] have conducted a lot of work to study
the effects of different repair parameters (scarf angle, lay-up, and adherend thickness) on the
performance of repaired laminated structures. They used three-dimensional (3D) finite element
(FE) models with cohesive damage to assess the strength of external adhesive repaired carbon-
fiber reinforced polymers (CFRP) under tensile and compressive loads [17, 20, 34]. The effect
of the shape geometry (single or double strap repair) on the strength of the structure and on the
stresses distribution in the repair joint has been particularly studied. They also developed two-
dimensional (2D) FE models for bonded repair joints [19, 20].The main conclusion was that
the repair strength increases exponentially with the decrease of scarf angle. Gunnion and
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Herszberg [21] developed 2D and 3D linear elastic parametric finite element models to analyze
stresses distribution in the middle of the adhesive joint of CFRP scarf repaired joints under
tensile loading. This model allowed obtaining both shear and peeling stresses distribution along
the adhesive bondline. A linear geometrical analysis was performed. The investigated
parameters included the adhesive and adherend thickness, the scarf angle and the stacking
sequence. The main conclusions of their study were the low sensitivity of the adhesive stresses
on mismatched adherends lay-ups and the major reduction in peak stresses observed when an
over-laminate ply was used to cover the full length of the specimen. Harman and Wang [14]
developed an analytical technique to optimize the shape of the scarf joints between dissimilar
adherends. Their technique used a linear variation of the scarf angle that generates a
characteristic scarf profile for a given adherends modulus ratio. Both analytical and 2D and 3D
elastic FE modelling results showed a dependence on the local ply orientation for peel and
shear stresses distribution in the adhesive, for different ratios of adherends moduli.
Charalambides et al. [16] tested experimentally repaired CFRP joints using a 2°-scarf
configuration. Distinct failure modes were observed as functions of the environmental
conditions (temperature and moisture) and of the load type. They also performed a two-
dimensional numerical analysis [15] in order to simulate three different failure modes in scarf
repairs: failure in the adhesive layer, failure induced from delamination initiating at the corner
of the overlap ply and tensile failure of the composite adherends. Failure loads were compared
with previously published experimental work, and the results were found to be in good
agreement.
173
The above-mentioned studies investigated repairs of composite laminates. Several
experimental studies and finite element analyses were also carried out to study the behavior of
repaired sandwich panels under four-point bending and compressive loads. The repair was
either extended across the width of the specimens (2D repair) [2, 47] or circular (3D repair)
[49, 50]. A series of experimental tests were conducted by Tomblin et al. [2, 51] to study the
effects of different process parameters on the quality of 2D repairs in sandwich panels. A
damage tolerance analysis of the sandwich structures was also included in their studies. As an
outcome of their work, a methodology for the repair process and the set-up of design tools for
damage tolerance analysis of sandwich structures were developed. On the other hand, Mahdi
et al. [47, 54] used 2D and quasi-3D finite element models to predict the performance of both
pristine and sandwich panels with 2D scarf repairs subjected to static and fatigue four-point
bending. Failure prediction was based on first ply failure using the Tsai-Hill criterion for the
composite skin, but failure of the adhesive was not considered. Numerical analysis results
showed a good correlation in terms of stiffness prediction of both undamaged and repaired
specimens. However, the predicted ultimate load was problematic and did not show a good
correlation with experiment. Ramantani et al. [52] studied also the performance of repaired
sandwich panels under four-point bending. They developed a 2D cohesive mixed-mode
damage model via interface elements placed along the adhesive bondline. Composite failure
was not considered. For overlap joints, they concluded that the repair strength increases as a
function of the overlap length and that the strength increases with lower scarf angles in the case
of scarf joints. The compressive behavior of sandwich panels with circular bonded repairs was
investigated by Liu et al. [49]. Both experiments and finite element analyses were conducted
174
to study the influence of repair variables such as scarf angle and cure cycle on the quality of
the repair. A progressive damage model, based on Hashin’s criterion for the composite
material, was developed and used to predict failure of the repaired sandwich panel. The
adhesive film was modeled using cohesive elements. Good correlation between experimental
and numerical results was obtained. However, it should be pointed out that since the inner
diameter of the repair was small (25 mm) compared to the sandwich panel width (100 mm),
the load was by-passed, and failure occurred in the parent and not in the adhesive bondline. A
very recent study from Zhang et al. [50] was conducted to investigate the mechanical
performance of honeycomb sandwich panels with open-hole damage and circular scarf repair
under compressive loads. A three-dimensional FE model was developed. Failure criteria based
on Hashin’s criterion with a progressive damage evolution were included for the composite
facesheets. The adhesive layer was modeled using cohesive elements and the honeycomb core
was considered as an elastic-plastic material. Good agreement was found in terms of ultimate
failure load and damage shape between the experimental and numerical results. Failure of the
repaired sandwich panel was due to adhesive delamination and patch local buckling. Another
finding of this work is that the structure strength increases with the decrease of the scarf angle
and that the optimum number of overply layers is one in order to reach the highest strength.
In the above-mentioned research works on sandwich repairs, focus was mainly on scarf-scarf
repair and failure of the adhesive film was taken into account using cohesive zone elements.
However, in practice stepped-scarf repair configurations are often used for which this
modelling technique cannot be applied. Hence, one of the aims of the present study is to account
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for the effect of the stepped patch on the adhesive peel and shear stresses distribution and
strength prediction.
This paper presents one aspect of a larger research program on the repair of sandwich structures
[80]. Here, the behavior of co-bonded circular scarf repair of sandwich composite panels under
edgewise static compressive and four-point bending loads is studied. Both experimental tests
and finite element analyses are performed. First, the repair procedure and the experimental set-
up are detailed. Force versus strain curves are presented and a series of failure morphology are
shown to determine the failure mode and pattern. Then, the FE models developed using the
commercial software Abaqus [56] are presented. Elastic-plastic analysis model with shear
failure for the adhesive coupled with the application of a failure criterion for the composite
skins is used to predict the ultimate load of the repaired sandwich structure subjected to
compressive loading. Finally, the numerical results are compared with experimental results to
validate the developed finite element models.
7.2 Experimental Work
7.2.1 Objective and Methodology
An experimental program has been set up to study the mechanical behavior of sandwich panels
with a circular flush repair on one of the two facesheets. A flush repair patch was selected over
an external repair patch because it offers structural strength as well as an aerodynamically
smooth surface. In practice, facesheets in sandwich structures work either in tension, in
compression or in shear. In this study, only the tensile and compressive behaviors of the
repaired facesheet were considered.
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To introduce a compressive load in the repaired facesheet, it was chosen to perform a
compressive test on the repaired sandwich panel. The test configuration allows having a clear
view of the circular repair as it is loaded in compression and digital image correlation systems
can therefore be used to measure the strains on the repaired facesheet. To load the repaired
facesheet in tension, a four-point bending test was preferred over a tensile test because it is
easier to conduct on large specimens and the specimens do not require any special preparation.
7.2.2 Specimen Preparation
The sandwich composite panels used in this work are composed of a Nomex honeycomb core
on which two out-of-autoclave four-ply plain weave (PW) carbon-epoxy skins are bonded
using a FM300-2M adhesive film. The cured composite ply thickness was approximately 0.19
mm and the film adhesive thickness was 0.25 mm. An over-expanded honeycomb core with a
19-mm thickness was used for the sandwich panels tested in compression. For the sandwich
beams tested under four-point bending load, a higher density hexagonal cell core with a 25.4
mm thickness was used to prevent core crushing from occurring. The elastic properties of the
composite material, the two Nomex honeycomb cores and the adhesive film are given in Tables
7-1, 7-2, 7-3 and 7-4, respectively. The inner facesheet, also called the tool facesheet, is a
[(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)] quasi-isotropic laminate. The outer facesheet, also called
the bag facesheet, has the same lay-up as the inner one. Specimens were tested under edgewise
compressive and four-point bending loads. Pristine, open-hole damaged and repaired sandwich
panels were tested under compressive loads. The hole was created to simulate damage that
177
could have been induced, for example, by impact. For the flexure tests, two configurations were
tested: pristine and repaired panels with the circular repair loaded in tension.
The pristine panel was manufactured as follows: both skins were bonded to the Nomex core
using the FM300-2M adhesive film and co-bonded under vacuum bag in an oven. For the
repaired and open-hole panels, the repair or the hole was carried out on the tool facesheet and
no core replacement was made. The hole and inner repair diameter was 50 mm. To simulate
material removal in the repaired skin, cut-outs were done in the prepreg plies with specific
diameters, so that, when stacked together, the prepreg plies formed a circular drop-off. The two
facesheets were bonded to the core using the same adhesive film as for the pristine panel. Next,
both skins and core were co-bonded under vacuum bag in an oven. The cure cycle consisted of
a four-hour room temperature vacuum hold followed by a two-hour 121°C dwell and a two-
hour post-cure at 180 °C. Vacuum-bag only pressure was applied during the whole cure cycle.
Then, the repair patch was manufactured as follows. After cure, the step-shaped parent area
was sanded with a 120-abrasive paper to reach the desired scarf angle (3o in this study). This
was followed by a surface cleaning with acetone and immediate drying. The repair patch was
prepared using the same prepreg material and stacking sequence as the parent skin. The plies
were cut to a specific diameter and stacked together to form an overlap as shown in Figure 7-1.
Next, the adhesive film and prepreg plies were applied directly over the prepared cut-out
surface. The patch and the parent were then co-bonded under a vacuum bag in an oven
according to the manufacturer recommendations.
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Figure 7-1 Stepped-scarf repair zone cross-section (not to scale).
Table 7-1 Mechanical properties of the plain weave composite material (CYCOM 5320
T650 PW).
E1t (GPa) E2t (GPa) G12 (GPa) ν12 ρ(kg/m3)
62.7 66.9 4.87 0.047 1500
E1c (GPa) E2c (GPa) X1t (MPa) X1
c (MPa) X2t (MPa)
49.3 48.7 999.7 772.2 875.6
X2c (MPa) S (MPa) G1t (N.mm-1) G1c (N.mm-1) G2t=G2c (N.mm-1)
789.7 38 22.5a 22.5a 22.5a
a Taken from [70]
Table 7-2 Mechanical properties of the over-expanded Nomex honeycomb core (ECA-R
4.8 64).
EW (MPa)
EL (MPa)
ET (MPa)
30.3a
0.089a
185a
GWL (MPa)
GWT (MPa)
GLT (MPa)
1.9b
55.5c
21.1c
WL
WT
LT
0.26b
0.22b
0.022b
a experimentally measured
b estimated from [64]
c from manufacturer
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Table 7-3 Mechanical properties of the hexagonal Nomex honeycomb core (ECA 3.2 96)
EW (MPa)
EL(MPa)
ET (MPa)
19.2
25.6
379.2
GWL (MPa)
GWT (MPa)
GLT (MPa)
5.13
68
96
νWL
νLT
νWT
0.85
0.020
0.224
a from manufacturer. The other values are estimated based on [64]
Table 7-4 Mechanical properties of the FM300-2M adhesive [76].
E (GPa) ν τy (MPa)
2.024 0.4 30
7.2.3 Edgewise Compressive Tests
Test Procedure
For the compressive tests, square test specimens were cut with a water jet-milling machine at
a nominal size of 203 mm by 203 mm. To prevent inadmissible ends failure and premature
failure, special considerations and panel preparations were made. A section of the core material
was removed at the top and bottom of the specimen and filled with a high stiffness potting
material to reinforce the edges. This section was 13 mm high and 203 mm wide. Aluminum
tabs were bonded at both ends to ensure a smooth load transfer in the potting-Nomex core
junction. Three strain gages were bonded on the specimens to detect possible bending due to
specimen misalignment and to study the strain distribution on the skins. Gage #1 was bonded
in the middle of the bag facesheet and the other gages (#2 and #3) were bonded on the tool
facesheet, as depicted in Figure 7-2.a. The surface of the specimen was also prepared for
measurement by a 3D digital image correlation (DIC) system (Aramis by GOM [73]). The DIC
post-processing software is used for the determination of the full in-plane and out-of-plane
displacements and strain field on the specimen surface during testing. The focus was directed
toward the front of the tool facesheet for the pristine, repaired and open-hole specimens.
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As a next step, the pristine, open-hole and repaired panels were subjected to edgewise
compression loading using an electromechanical MTS testing machine with a 250 kN load cell
at a constant crosshead rate of 0.5 mm/min. Specimens were placed in a compressive test
fixture, similar to the fixture recommended by the ASTM D7137 [81] for compression after
impact, as shown in Figure 7-2.b. These tests were performed in order to compare the
mechanical performance of repaired panels versus pristine and open-hole damaged panels.
Table 7-5 summarizes the test matrix conducted for each configuration. The stress in the skin
was evaluated according to
2 f
Ft W
(42)
where F is the force recorded during the test, tf is the skin thickness and W is the width of the
specimen.
Test Results
The stiffness and strength obtained for the static compressive tests performed at ambient
temperature on the pristine, open-hole and repaired coupons are listed in Table 7-6. As can be
seen from the table, sandwich panels with open-hole have the lowest compressive strength due
to the high stress concentration around the edges of the hole and the strength recovery was only
about 45%. However, higher strength recovery was obtained after repair. Compared to the
pristine sandwich panels, the strength recovery of repaired panels reaches about 85 %. This
high strength recovery indicates that the repair process conducted on the sandwich panel can
restore efficiently its mechanical performance.
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Table 7-5 Test matrix.
Skin material Pristine
Specimens
Open-hole Specimens Repaired
Specimens
Plain Weave (PW) 4 2 3
Figure 7-2 Compressive test fixture and strain gages location.
7.2.4 Four-Point Bend tests
Test Procedure
Long-beam flexure tests were performed on the pristine and 3°-repaired sandwich beams in
accordance with the ASTM standard D7249 [83] standard. The test fixture and the specimen
dimensions were carefully selected to ensure that failure occurs in the composite facesheets
and to prevent core shear failure. As shown in Figure 7-3, the load span (L) and the support
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span (S) were taken equal to 153 mm and 660.4 mm respectively. The pristine sandwich beams
were 76.2 by 686 mm2 and the repaired sandwich beams were 203 mm wide and 686 mm long.
Specimens were tested, at room temperature conditions, using an electromechanical MTS test
frame with a 100 kN load cell. A crosshead rate of 8 mm/min was used for these tests. Strains
gages and a digital image correlation (DIC) system [73] were used to measure the strains on
the specimens. Here, the repaired facesheet was loaded under tension.
The stress developed in the facesheets was calculated according to ASTM standard D7249
standard using:
( - )
2( )c f
P S Ld t Wt
(43)
where F is the force applied during the test, tc is the core thickness, d is the measured total
thickness of the sandwich panel, W is the width of the specimen and tf is the facesheet thickness.
Test Results
Figure 7-4 and Figure 7-5 show the flexure stress-strain responses for the pristine and repaired
sandwich beams with the repair loaded in tension. It can be observed from the figures that the
flexure response is linear until failure occurs suddenly. Moreover, all the observed failure
modes for the pristine and repaired beams were fiber fracture, away from the load points, on
the side loaded in compression, as shown in Figure 7-6. Therefore, failure occurred in the
middle of the pristine bag facesheet, loaded in compression, and not in the repaired facesheet.
This failure mode shows the efficiency and the high strength recovery of sandwich panels with
circular repair loaded in tension.
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Figure 7-7 recapitulates the flexure failure stress for the pristine and repaired panels. It can be
observed that when the repair is loaded in tension, a higher strength recovery was obtained,
around 95% of the pristine value.
Table 7-6 Test results for different sandwich panels configuration.
Specimen
configuration
Specimen
number
Scarf
angle (°)
Stiffness
(GPa)
Failure stress
(MPa)
Strength
recoverya (%)
Pristine 4 - 40.03 374.40 100
Open-hole 2 - 36.88 169.66 45.31
Repaired 3 3° 41.91 318.47 85.06
a Strength recovery (%)= 𝜎𝑓
𝜎𝑝𝑟𝑖𝑠𝑡𝑖𝑛𝑒𝑓 × 100
Figure 7-3 Specimens configuration and four-point bending test fixture.
184
Figure 7-4 Stress-strain curves for the pristine sandwich beams.
Figure 7-5 Stress-strain curves for the 3° repaired sandwich beams.
185
Figure 7-6 Failure morphology of the pristine and the 3°-repaired sandwich beams under
four-point bending.
Figure 7-7 Failure stress of the pristine and 3° repaired panels under four-point bending.
7.3 Numerical Simulation
7.3.1 Finite Element Model Description
The finite element software Abaqus/Explicit was used to predict the response of the repaired
sandwich panels under edgewise compressive loading. The behavior of the repaired sandwich
beam under four-point bending was not modelled since the repair did not fail for this test. Three
different configurations were studied just like the experimental tests, i.e., pristine, open-hole
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and repaired panels. Each FE model involves three components: the tool facesheet, the Nomex
core and the bag facesheet. As, the specimen for all tested configurations is symmetric, only a
quarter of the panel was modeled. So, the panel quarter dimensions were 102 mm long, 102
mm wide and 20.52 mm thick. For both repair and open-hole specimens, the repair and open-
hole zones have finer meshes. The adhesive film along the bondline was discretized through
the thickness using four continuum solid elements (C3D8R and C3D6R). Each single woven
ply was discretized through the thickness using one thick continuum shell element (SC8R).
The Nomex honeycomb core was also discretized through the thickness using at most five
continuum solid elements (C3D8R) as shown in Figure 7-8.
For the repaired panel, a refined mesh was used for the patch and adhesive edges where strain
gradients occur (Figure 7-9). To ensure mesh matching, the parent, the patch, the adhesive and
the core were discretized with the same in-plane mesh density. A mesh convergence study was
conducted to verify the accuracy of the finite element models. Here, the total elastic strain
energy was used as indicator (ALLSE in Abaqus [56]). Considering the complexity of the FE
model, the zones that have the highest percentage of strain energy were identified and then
were progressively refined.
Bonding between the composite facesheets and the Nomex core was assumed perfect and a tie
constraint was applied at the core/facesheet interface. Also, the contact between the adhesive
film and the core was considered perfect and a tie constraint was applied. The facesheets had
the same lay-up as in the experiments [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)] and each single ply
had a thickness of 0.19 mm. The Nomex honeycomb core had a thickness of 19 mm. The
mechanical properties of the composite materials used for the sandwich panels are summarized
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in Table 7-1. The mechanical properties of the adhesive film are indicated in Erreur ! Source
du renvoi introuvable. and the elastic properties of the Nomex honeycomb core are listed in
Table 7-2.
For the current finite element analysis, the honeycomb core is assumed to behave as an
orthotropic linear elastic material. The adhesive film behavior is described using an isotropic
elastic plastic model and a shear failure criterion is used to predict the adhesive failure. The
composite material is modeled as an orthotropic elastic material with progressive stiffness
degradation and plastic deformation under shear loading. Delamination was not taken into
account.
The boundary conditions are defined as indicated in Figure 7-10. On the bottom edge,
symmetry conditions along the y-axis were imposed, on the free top edge, a compressive
displacement, as measured from the experiment, was applied. The out-of-plane displacements
were constrained on the right edge side blocked by the fixture along the in-plane direction of
the model and symmetric conditions along the x-axis were applied.
Figure 7-8 Mesh details of the honeycomb sandwich panels.
188
Figure 7-9 Mesh refinement details of the 3°-repaired panel
Figure 7-10 Boundary conditions applied in the finite element model.
7.3.2 Failure Criteria and Damage Evolution
Composite Material
Progressive damage of the woven fabric composite skins of the sandwich panels was modelled
in the Abaqus/Explicit environment [56]. The continuum damage mechanics model is based
on the built-in user’s material subroutine called ABQ-PLY_FABRIC, proposed by Johnson et
al [69], for 2D woven fabric composites. The quasi-isotropic laminate is modeled by stacking
Parent
Adhesive
Patch
Patch mesh details
through thickness
Ply 4
Ply 3
Ply 2
Ply 1
Ply 1
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layers of continuum shell elements with reduced integration (SC8R) through the thickness. The
laminate is composed of four plies each displaying an orthotropic behavior with progressive
damage. The behavior of a damaged ply is described by the following stress-strain relation in
the local material coordinate system (1, 2):
12
1 1 111 11
2122 22
2 2 2
12 12
12 12
1 0(1 d )
1 0(1 d )
10 0(1 d )
E E
E E
G
(44)
where E1, E2 are the initial undamaged elastic moduli respectively in the warp and weft
directions of the woven fabric, ν12 is the in-plane Poisson’s ratio and G12 is the undamaged in-
plane shear modulus. The damage variables d1, d2 and d12 are associated with the warp- and
weft-directions and the in-plane shear failure, respectively.
For woven fabric composite materials, it is assumed that there are two main failure mechanisms
[69]:
- Fiber-dominated failure in tension or compression in the two fiber directions,
- Matrix failure in in-plane shear.
In order to take into account both tension and compression stiffness in the model, the elastic
values E1, E2 are assumed to take their compressive or tensile values depending on the sign of
tr(ε)=ε11+ε22. The built-in subroutine offers two different options to delete elements from the
model:
190
- The element is deleted when d1=dmax or d2=dmax under compressive or tensile load, or
when the plastic strain due to shear deformation reaches the maximum value, 𝜀𝑝𝑙 =
𝜀𝑚𝑎𝑥𝑝𝑙
- The element is deleted when d1=d2=dmax along both fiber directions, or when the plastic
strain due to shear deformation reaches the maximum value, 𝜀𝑝𝑙 = 𝜀𝑚𝑎𝑥𝑝𝑙
In this study, the first option to delete elements was used. To reduce the time required to
complete the simulation of the quasi-static compressive test using Abaqus/Explicit, the mass
scaling technique was used, following guidelines described in Abaqus user’s manual [56]. To
ensure that there is no influence of the artificial mass added to the system on its global physical
response, the injected kinetic energy of the whole model was verified, and it was less than 5%
of the internal energy of the whole system. So, mass scaling has no major effect in the obtained
results.
Adhesive Film Material
The adhesive film was not modeled using cohesive elements as it was the case in previous
studies from the literature [49, 50, 52]. Cohesive zone model are based on several parameters
that are difficult to measure and that are often estimated by trial and error. Instead, 3D solid
elements were used to discretize the adhesive. These elements used in conjunction with an
elastic-plastic material model and the von Mises yield criterion allow to predict the elastic-
plastic behavior of the adhesive [76]. The material mechanical properties required for the model
were determined experimentally. A shear failure criterion was also associated with the von
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Mises yield criterion to predict the adhesive failure. This criterion is based on the value of the
equivalent plastic strain at element integration points. Failure is assumed to occur when the
damage parameter w exceeds one. This damage parameter is defined as:
pl
pl
f
w
(45)
where 𝜀 ̅𝑝𝑙 is the equivalent plastic strain and designated as PEEQ in ABAQUS/Explicit, ∆𝜀 ̅𝑝𝑙
is the increment of PEEQ and 𝜀�̅�𝑝𝑙
is the plastic strain at failure. When the shear failure criterion
is reached at an element integration point, the material is assumed to fail at this point and the
stress components are set to zero. The element is deleted from the mesh when the material
failure is detected at all integration points.
7.3.3 Results and Discussions: Edgewise Compressive Tests
Stiffness and Strength
Figure 7-11.a to Figure 7-11.c show the compressive stress-strain curves for the pristine, the
open-hole and the 3°-repaired sandwich panels. As can be observed from these curves,
experimental and numerical results are fairly similar. This indicates that the finite element
model can accurately predict the compressive behavior of the pristine, open-hole and repaired
sandwich panels. We can also observe that for all tested specimens, the stress-strain curves are
linear until failure which occurs suddenly (when the maximum value is reached). It is worth
noting that the ultimate strain reached for the repaired panels far exceeds the design ultimate
strain requirements of the order of 5000 µε usually used in the aeronautical industry [84].
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Failure Mode and Damage Shape
The experimental fractured surfaces of pristine, open-hole and repaired sandwich panels are
shown in Figure 7-12.a to Figure 7-12.c. Figure 7-12.a shows the damage shape of the pristine
panels after compressive loading. It can be observed that damage occurs mainly at the top and
bottom ends near the support and loading zones. This may be explained by the non-uniform
loading experienced in these zones. Figure 7-12b shows the ruptured facesheet of an open-hole
specimen. Damage expands from the equators of the open-hole to the unloaded ends of the
panel. The failure mechanism was similar for all open-hole panels. This can be explained by
the high stress concentration that occurs at the equators of the open-hole. Figure 7-12.c shows
the ruptured facesheet for the 3°-repaired panels for which failure occurred mainly along the
top edge of the patch and that expanded to the unloaded parent ends. Figure 7-13.a to Figure
7-13.c show the failure morphology of the three configurations obtained from the numerical
predictions. It can be observed that the predicted damage shape is in accordance with the
experimentally observed failure morphology for each configuration. From the numerical
simulation, failure occurs according to the following scenario. For the pristine panel, rupture
occurs mainly near the loading edges, where stress concentration is present. It was found that
failure occurs in the 0°-plies in compression. Then, matrix failure occurs immediately followed
by total failure of the specimen. For the open-hole specimen, failure occurs also in the 0°-plies
and propagated to the other plies. For the 3°-repaired specimens, failure occurs first in the
adhesive bondline located under the patch, then failure propagates through the adhesive and
finally the 0°-plies located in the parent side fail in compression. Finally, failure occurs
simultaneously in the other plies which leads to the global failure of the specimen.
193
a. Pristine panels.
b. Open-hole panels.
c. 3°-repaired panels.
Figure 7-11 Finite element prediction versus experiment results for composite sandwich
panels
194
Figure 7-12 Failure mode for the tested composite sandwich panels.
Figure 7-13 Predicted failure morphology for the three panel configurations.
195
7.4 Conclusion
This study investigated bonded repairs in composite sandwich panels made with honeycomb
core and out-of-autoclave woven prepreg carbon-epoxy skins. Experimental tests were carried
out to investigate the compressive behavior of pristine, damaged and repaired sandwich panels.
Flexure tests were also conducted to study the behavior of the repaired skin loaded in tension.
Experimental results indicate that the repair configuration can recover up to 85% of the static
mechanical strength of the pristine panels for a 3°-stepped-scarf patch under compressive loads
and can recover up to 95% of the pristine value under flexure loads with the repair loaded in
tension. These results show the high ability of the circular repair to restitute the pristine strength
value. Also, it has been observed that the circular repair loaded in tension is stronger than when
it is loaded in compression.
3D finite element analysis models were proposed in the paper to predict the behavior of pristine,
damaged and repaired sandwich panels under compressive loads. Good agreement between
stiffness and strength predictions and experimental results confirmed that the developed
numerical model provides an effective analysis tool for the mechanical behavior prediction of
repaired composite sandwich panels.
This study investigated the mechanical behavior of bonded repairs in composite sandwich
panels under room temperature conditions. However, bonded repairs are exposed to different
environmental conditions (cold, hot/wet conditions) during their service life which will affect
their long-term performance. The effects of environmental conditions on the mechanical
196
behavior of bonded repairs must be accounted for in the design and will be investigated in a
follow-up study.
Acknowledgements
We would like to thank the Natural Sciences and Engineering Research Council of Canada
(NSERC), the Consortium for Research and Innovation in Aerospace in Quebec (CRIAQ), the
National Research Council Canada (NRC), Bombardier Aerospace and L3-MAS for funding,
technical support and materials.
197
Chapter 8.
Conclusions and Perspectives
8.1 Thesis Conclusions
The general objective of this study was to propose a reliable bonded repair methodology for
primary sandwich honeycomb structures for aerospace applications, and particularly through
the development of numerical tools and protocols for the design of sandwich composite bonded
repairs. For that purpose, a series of experimental investigations and numerical simulations of
repaired bonded honeycomb sandwich panels were conducted. The following approaches were
taken to address the problem:
Assessment of the mechanical behavior of honeycomb sandwich panels with
bonded repairs by experimental testing.
Development of finite element models for better understanding and accurately
predicting the mechanical behavior and the failure modes of the repaired
sandwich panels under different loadings.
Validation of the finite element models and conduction of a parametric study.
This report has presented an experimental and numerical investigations of the mechanical
performance of stepped-scarf repairs in composite honeycomb sandwich panels under different
loading: tension, compression and four-point bending. The finite element models have been
conducted for predicting the strength and failure mode of repaired composite sandwich panels
198
with two repair configurations: 2D repair and 3D repair. These models have been
complemented by experimental studies which provided data for model validation. The
experimental study revealed that the repaired sandwich panel with the repair facesheet loaded
in tension is stiffer than the repaired sandwich panels with the repair loaded in compression.
The finite element model generally agreed well with the failure stress and mode observed in
the experiments for these different configurations.
In chapter 1, a state of the art literature review allowed to point out the need and the importance
of developing a novel methodology for bonded repair of woven composite sandwich primary
aircraft structures. In particular, the following issues were highlighted:
The use of out-of-autoclave woven fabric materials are scarcely discussed in the
literature.
The modelling of a real repair geometry; stepped-scarf configuration by the finite
element method and the study of the effect for different geometric design parameters in
the repair strength were seen to require further studies in order to develop a reliable
analytical tool for current and future bonded repairs of advanced composite aircraft
structures.
Chapter 2 presented the thesis objectives and the methodology used to achieve them.
Chapter 3 presented the experimental work performed to determine the mechanical properties
of the sandwich materials constituents, namely the composite facesheets and the core. First, the
tensile and compressive tests allowed to determine the in-plane properties of the composite
materials. It was observed that the two PW and 8HS composite materials had similar
199
mechanical behavior under tension and compression. Also, the elastic in-plane tensile and
through-thickness compressive moduli of the Nomex core were determined. From the test
results, it was observed that the over-expanded core was stiffer in the W-direction. The
mechanical behavior of the core under failure needs however further investigation. Then, 2D
and 3D finite element models were developed and validated by comparing the predicted
mechanical behavior of a quasi-isotropic laminate with results from experiments and classical
lamination theory. The finite element predictions showed a good agreement with both CLT and
experiments in terms of stiffness when the CPEGI elements from Abaqus library were used.
The 3D model takes into account the progressive damage failure of woven fabric facesheets
and showed a good correlation in terms of the failure stress. Further improvement could be
achieved by developing more elaborated models taking into account the experimental
variability.
In Chapter 4, results on the experimental and numerical investigations conducted on the 2D
repaired sandwich panels under tensile loading were presented. The effect of varying the scarf
angles (3°, 5°, 7°) was studied and it was shown that for a rectangular repair patch across the
plate specimen, a 2D plane strain FE model can predict reasonably well the mechanical
behavior of the repaired structure until failure. The main achievement of this work was that
with the use of an elastic-plastic behavior of the adhesive film with a shear failure criterion, we
could accurately predict the failure stress and mode of the tested specimens. Also, from both
numerical simulations and experiments, it was observed that there is no major effect of the
scarf angle on the strength recovery, for angles from 3° to 7°. Further investigations should be
considered to determine the effect of the scarf angle under various environmental conditions.
200
In Chapter 5, a parametric study on the strength recovery of 2D repaired panels was conducted.
The effect of different geometric parameters (scarf angle, number of plies and skin thickness)
on the strength recovery of the repaired panels was studied under tensile loads and it was found
that the addition of one (+45/-45) overply improved the strength of the repair by 40% in
comparison with the case when no overply was used. Another finding from this work was the
important effect of the skin thickness on the strength recovery. Thick skin sandwich panels
(eight-ply skin panel) showed a much higher strength recovery in comparison with thin one
(two-ply skin panel). The failure was no more in the adhesive but in the composite part of the
structure.
In Chapter 6, the experimental and numerical investigations performed on 2D repaired panels
were extended to study their behavior under edgewise compression and their behavior using a
four-point bending load configuration. Here, a comparison between four-point bend, and
edgewise compressive tests was presented. Four-point bend tests require longer specimen but
are easier to perform than compressive tests to determine the mechanical behavior of the
sandwich panel for a repair loaded in compression.
In Chapter 7, circular repaired sandwich panels were studied experimentally and numerically.
First, the behavior of repaired specimens under compressive load was determined
experimentally. The behavior of the circular repair under tension was then determined by
conducting a four-point bending test with the repair on the bottom beam surface. Results show
that 85% of the strength was recovered when the repair is loaded in compression and about
90% was recovered when the repair is loaded in tension. These results show the ability of the
developed repair technique to restore a high level of the pristine strength. Then, the
201
development and implementation of a 3D finite element model with a progressive damage and
failure model for the woven fabric composite was carried out to predict the stiffness and failure
mode of the repaired sandwich panels under compression. The finite element predictions were
in good agreement with the experimental results, which confirms that the developed finite
element model may be used as an alternative tool to study the mechanical behavior of repaired
sandwich structures.
8.2 Thesis Original Contributions
This project achieved its primary objectives of:
Assessing the mechanical behavior of repaired composite sandwich panels under
different loads: tension, compression and four-point bending.
Proposing a finite element model for repaired composite sandwich panels that can
reliably produce good estimates of the failure strength and mode for different repair
configurations (rectangular and circular repairs) and under different loads (tension,
compression and four-point bending) while considering all the major design parameters
of repaired composite sandwich panels.
This study presents a comprehensive investigation on methods of characterization of out-of-
autoclave stepped-scarf repaired composite sandwich panels. The development of finite
element modelling technics and experimental methods for characterization and validation of
the mechanical performance of repaired panels were presented through extensive review of
reported studies on both repaired monolithic and sandwich composites structures. The review
covered different static characterization methodologies, analytical formulations and finite
202
element modelling technics. Also, the effect of various geometrical design parameters on the
strength recovery of the repaired structure addressed in earlier studies were thoroughly
discussed. The major contributions of the research work are summarized as follows:
A FE model describing and predicting the mechanical behavior of the stepped-scarf
repair on sandwich honeycomb panels with different configurations under different load
cases (compression, tension, four-point bending) was developed.
The finite element models provide a simple tool and a good alternative to predict the
mechanical behavior of the stepped-scarf repaired sandwich panels under different load cases.
Overall, the FE calculations successfully predicted the failure strength and mode of the repaired
sandwich panels. The stepped-scarf repair patch, like the one performed experimentally, was
studied and a better understanding of the adhesive joint’s behavior is provided. The determination
of the stress distribution along the adhesive bondline helped to understand the failure mode that
occurs. Good agreement between stiffness and strength predictions and experimental results
confirmed that the developed numerical model provides an effective analysis tool for the
mechanical behavior prediction of repaired composite sandwich panels. These models have been
developed based on the physical parameters of the adhesive film.
A better understanding of the geometrical design parameters effects on the mechanical
performance of the sandwich repaired panels
A guideline for the design of stepped-scarf repair was conducted with a parametric
study using the developed FE model and allows to study the effect of different geometric
parameters on the strength recovery of the repaired sandwich structure. This guideline may
give instructions and better understanding for the choice of the scarf angle, the number of
overply depending on the sandwich structure to be repaired. An interesting finding here is the
203
influence of the skin thickness on the repair strength recovery. Thin skin sandwich panels are
very sensitive to the repair and small scarf angle should be used. The addition of an overply is
primordial for thin skins. From the parametric study, the use of an overply shows a higher
strength recovery and a change in the failure mode of the repaired panels. This result was
validated by experiments.
A determination of a database of mechanical properties for out-of-autoclave (OOA)
composites materials for repairing primary aerospace honeycomb sandwich structures
A comprehensive review of reported studies on experimental methods for the
characterization and determination of the mechanical performance of repaired sandwich panels
were conducted. An experimental characterization program was developed to identify the
performance of the repaired panels under different load cases (compression, tension, four-point
bend). Furthermore, the complexities associated with the experimental characterization and
disagreements between experimental results from the different tests were addressed. To
demonstrate the validity of the different results, a comparison was made in terms of the
stiffness, failure stress and mode. Considering this, a first database of the mechanical
performance of repaired sandwich panels was developed on the basis of the different
mechanical tests results and compared to the predicted calculation from the finite element
models. At our best knowledge, this is a first database about these new out-of-autoclave
composite materials (PW and 8HS), as a candidate for repairing honeycomb sandwich primary
structures, to be completed at room temperature conditions. These materials are expected to be
increasingly used in the aerospace applications and had not been used yet for repairs of
composite primary structures.
204
8.3 Recommendations for Future Work
From the above indicated conclusions and contributions, one then deduces that the following
issues need further investigations. In short terms, in order to complete the work presented here,
the following works should be accomplished:
The parent structures and repairs were cured out-of-autoclave in an oven. More
investigations of the mechanical behavior of co-bonded repaired composite sandwich
panels using a hot-bonder or heat blanket need to be assessed and compared with the
mechanical performance for a co-bond cured in oven.
The mechanical performance was conducted under static loads. So, it is important to
understand the behavior of the repaired composite sandwich panels under dynamic
loads.
Aerospace structures are very sensitive to impact damage. Hence, a sensitivity study
of the repaired patch to impact damage should be undertaken in the short and long-term
range.
The compression-after-impact (CAI) should be used to assess the performance of
impacted repaired composite sandwich panels using both numerical and experimental
methods.
As a long-term work, it would be interesting to eventually assess eventually the developed
methodology as a potential candidate for field repair technology of advanced woven composite,
by further investigating the following issues:
205
The rectangular and circular repaired sandwich panels have been tested at room
temperature conditions. Environmental conditions have not been included in this work.
As the mechanical properties of the adhesive film are very affected by temperature and
humidity, tests under different environmental conditions (cold, hot and humid) should
be conducted to determine the performance of the repaired panels under in service
conditions.
Fatigue and ageing of bonded repair structures are still an open issue and should be
considered for further investigations.
As the repaired panels are co-bonded using a heat blanket or hot bonder in practice,
measurement and identification of thermal residual stresses may be an important point
to be considered.
A modification of the developed finite element model to consider the thermal residual
stresses may be necessary to estimate the residual stress effect in the repair mechanical
performance.
206
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Appendix A.
Mechanical performance of the 8HS honeycomb
sandwich panels
With the increasing use of composite materials in aerospace primary structures, the need for
reliable repair methods is growing in the aeronautical industry. In this research work, an
investigation of OOA prepregs as potential candidates to produce stepped-scarf bonded repairs
on sandwich honeycomb panels, with only vacuum bag pressure, was conducted. The main
objective was to better understand the mechanical performance of the repaired sandwich panels
in function of skin material morphology (architecture), geometric design parameters and
applied load cases. This appendix is dedicated to the presentation of performed experimental
tests in order to determine the mechanical performance of repaired sandwich panels with
different prepreg composite skin material for the case of eight harness satin material (8HS).
A.1 Tensile Tests on Pristine and Repaired 8HS Honeycomb
Sandwich Panels
The 8HS honeycomb sandwich specimens were tested in tension, at room temperature
conditions, as for the PW panels. Two main groups of specimens were prepared to determine
the tensile properties of the panels. Namely, three 2D repaired coupons with 3° scarf angle and
three pristine panels for the strength recovery comparison.
213
Specimens Dimensions and Test Set-up
The pristine and the repaired 8HS sandwich panels considered in the experimental studies were
335 mm long, 102 mm wide and 22.04 mm thick. Tensile tests were performed using the same
set-up and the same displacement rate of 2 mm/min as for the PW panels. Here, both the DIC
system and the video extensometer were also used to measure the deformation of the panels,
as shown in Figure A-1.
The repaired panels had also a double step-scarf joint. The repair was carried out on the tool
facesheet. The sandwich panels were composed of an over-expanded Nomex honeycomb core
with a 19-mm thickness on which two four-ply carbons-epoxy skins were bonded. The skin
was made with an out-of-autoclave plain weave prepreg (CYCOM 5320 T650 8HS from Cytec
Engineering Materials) with a 0.38 mm thickness. The ply stacking sequence for the tool
facesheet is a [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)]. The bag facesheet has the same lay-up as
the inner one. The patch repair has also the same lay-up as the parent structure. The skin 0°-
direction is aligned with the x-direction. The ribbon direction of the Nomex core is
perpendicular to the x-direction. The repair patch is bonded to the parent structure by the same
adhesive film (FM 300-2M from Cytec) with a 0.25 mm thickness, placed along the scarf and
under the patch.
214
Figure A-1. Tensile test set-up for 8HS sandwich panels
Test Results for the Pristine 8HS Honeycomb Sandwich Panels
The results of the static tensile tests performed at ambient temperature on the pristine sandwich
panels, are presented in Figures A-2 and A-3. Figure 2 presents the load versus strain measured
on the tool facesheet using the DIC system for the pristine panels. It can be observed from these
figures that the load-strain behavior is mostly linear until failure for both pristine panels. Figure
A-3 presents the load-strain curves measured on both the tool and the bag facesheets for one
pristine specimen. The uniform load distribution in both facesheets can be assessed by the
similarity in strains measured by both the DIC system and the video extensometer.
Test Results for the 2D Repaired 8HS Honeycomb Sandwich Panels
Here, only 3°-repaired 8HS panels were tested under tensile loads, at room temperature
conditions. Figure A-4 presents the load-strain curves measured on the tool face sheet with the
215
DIC system for the 3°-repaired specimens. It can be observed, as for the pristine panels, that
the behavior of the tested repaired panels is linear until the occurrence of the brittle failure.
Figure A-2. Load-strain curves of the tensile tests of the pristine 8HS sandwich specimen
Figure A-3. Comparison of the axial load-strain curves obtained on both facesheets of the
8HS pristine sandwich specimen.
216
Figure A-5 presents the load-strain curves measured on both the tool (repaired) and the bag
facesheets for one 3°-repaired specimen. The uniform load distribution in both facesheets can
be assessed by the similarity in strains measured by both the DIC system and the video
extensometer. For the 3°-repaired panels, failure occurred mainly in one of the two scarf zones.
This failure is similar to the 3°-repaired PW panels failure.
Figure A-4. Axial load-strain curves obtained for the 3°-repaired 8HS sandwich specimens
(strains measured by DIC on the tool facesheet (repaired facesheet)).
217
Figure A-5. Comparison of the axial load-strain curves obtained on both facesheets of the 3°
repaired 8HS sandwich specimen.
Strength Recovery of the 3°-Repaired Sandwich Panels
The test results for the pristine and for the 3°-repaired 8HS specimens are summarized in Table
A-1. Figure A-6 compares the experimental failure strength (σf) obtained for the 3°-repaired
panels with that measured for the pristine panel. As it can be observed from this figure, the
failure strength is about 60.20 % of the pristine value. The strength recovery for this sandwich
repair configuration is quite low. However, it is quite higher than the value obtained for the
PW repaired panels (55 %). Using an over-ply could be beneficial to improve the strength of
the repaired 8HS sandwich panel as for the PW repaired sandwich panel.
Table A-1. Tensile results for 8HS sandwich panels
Configuration Angle
(°)
Elastic modulus
(GPa)
Failure strength
(MPa)
Strength recovery
(%)
8HS-Pristine - 45.90 488 -
8HS-Repair 3 46.48 293.42 60.12
218
Figure A-6. Tensile failure stress of the pristine and 3°-repaired sandwich specimens.
A.2 Compressive Tests on 8HS Honeycomb Sandwich Panels
As a next step, static edgewise compressive tests were performed in order to compare the
compressive performance of the repaired panels with that of the pristine panels. As for PW
materials, two sets of sandwich panels were considered: one with three 8HS pristine specimens
and the other with three 8HS repaired specimens. Special considerations and panel preparation
were made as for the PW panels. Strain gauges and DIC system were also used to measure the
strain of both the tool and the bag facesheets of the specimens, as illustrated in Figure A-7. As
for PW material, two repair configurations were tested: the 2D rectangular shape repair and the
3D circular patch repair.
219
Compressive Tests on Pristine and 2D Repaired Honeycomb Panels
A.2.1.1 Compressive Tests on the Pristine 8HS Honeycomb Sandwich Panels
The 8HS pristine specimens were tested to failure under compressive loading, at room
temperature conditions. Specimens were cut, in a rectangular shape, by water jet at a nominal
size of 305 mm by 102 mm. The compressive test results are presented in Figures A-8 and A-
9. The load-strain curves for the pristine panels are shown in Figure A-8. It can be observed
from this figure that the load-strain curve is mostly linear until a sudden failure of the panel.
Different measurements of the load versus strain, obtained with various instruments, are shown
in Figure A-9. The uniform load distribution in both facesheets can be assessed by the similarity
in strains measured by different instruments (strain gages and DIC), as for the tensile
specimens. It should be noted also that all the failure zones were located away from the loaded
ends.
Figure A-7. Strain gages locations on the tested specimens
220
Figure A-8. Force versus strain curves of pristine panels
Figure A-9. Force versus strain curves measured by different instruments on both facesheets
of the pristine sandwich panel
221
A.2.1.2 Compressive Tests on the 2D Repaired 8HS Honeycomb Sandwich Panels
The compressive test results are presented in Figures A-10 and A-11. The load versus strain
curves obtained for the 3°-repaired panels are shown in Figure A-10. It can be seen from the
figure that the load-strain curve is mostly linear until the occurrence of a sudden failure, as for
the pristine panel. A good repeatability was also observed for the test. The difference in the
load carried by the pristine and the repaired facesheets can be seen by the difference in strain
measured by gage 1 and DIC versus that measured by gage 2, as illustrated in Figure A-11. The
failure mechanisms were similar for all the repaired specimens. Local buckling in the scarf area
was observed, as it was the case for the PW repaired sandwich panel.
Figure A-10. Force versus strain curves of 3°-repaired panels
222
Figure A-11. Force versus strain curves measured by different instruments on both facesheets
of the 3° repaired sandwich panel
A.2.1.3 Recapitulation and Strength Recovery of the 8HS Repaired Sandwich
Panels
Three scarf angles were tested here: 3°, 5° and 7°. Table A-2 summarizes the results of the
tested specimens and the strength recovery for each scarf angle. It can be observed that the
strength recovery increases as the scarf angle increases. From the DIC measurement, local
buckling of the repaired facesheet was observed for the 3°, 5° and 7° repaired specimens, as
can be seen in Figure A-12. This failure mode may explain the fact that the strength recovery
increases with the increase of the scarf angle. Similar results were also observed for the PW
material panels. Figure A-13 compares the experimental failure strength (σf) for different scarf
angles for both PW and 8HS materials with the pristine panels. As can be observed, the failure
stress of the 3°-repaired PW panel is lower than the 3°-repaired 8HS panel. However, the
223
strength of the 5°-and 7°-repair panels increases at a slower rate than for the PW repaired
panels.
Table A-2. Compressive results for 8HS sandwich panels
Configuration Angle
(°)
Elastic modulus
(GPa)
Failure strength
(MPa)
Strength recovery
(%)
8HS-Pristine - 40.46 376.01 -
8HS-Repair
3 36.78 232.25 61.76
5 36.18 233.41 62.07
7 37.16 245.39 65.26
Figure A-12. Typical failure mode of 3°-, 5°- and 7°-repaired 8HS sandwich panels under
edgewise compressive load
224
Figure A-13. Comparison of the compressive strength for PW and 8HS sandwich panels
under edgewise compressive load
Compressive Tests on 3D Repaired and Open-Hole 8HS Honeycomb
Panels
Two different configurations were tested under edgewise compressive loads: two open-hole
panels and two 3-repaired panels. For the open-hole panel, a hole diameter of 50 mm was used.
Specimens were cut, by water jet at a nominal size of 203 mm by 203 mm. The repair was
carried out on the tool facesheet. The patch repair is a four-ply carbon-epoxy laminated
composite. The skin is made with an out-of-autoclave plain weave prepreg (CYCOM 5320
T650 8HS from Cytec Engineering Materials) with a 0.38 mm thickness. The ply stacking
sequence for the tool facesheet is [(+45/-45)/ (0/90)/ (-45/+45)/ (90/0)]. The bag facesheet has
the same lay-up as the inner face.
225
The compressive test results for both the repaired and the open-hole specimens, are presented
in Figures A-14 and A-15, respectively. It can be observed from these figures that the load-
strain curves are mostly linear until sudden failure for both configurations. Figures A-16.a and
A-16.b show the ruptured facesheet of an open-hole and a repaired specimen, respectively. For
the open-hole panel, damage expands from the equators of the open-hole to the unloaded ends
of the panel. The failure mechanism was similar for all the two tested panels. This can be
explained by the high stress concentration that occurs at the equators of the open-hole. Figure
16.b shows the ruptured facesheet for the 3°-repaired panels for which failure occurred mainly
along the top edge of the patch and that expands to the unload parents ends.
The results of the static compressive tests performed, at ambient temperature, on the pristine,
on the open-hole and on the repaired specimens are listed in Table A-3. As can be seen, 8HS
sandwich panels with open-hole have the lowest compressive failure strength due to the high
stress concentration around the edges of the hole and the recovery was only about 43%. Higher
failure strength was obtained for the repaired specimens. Compared to the pristine sandwich
panels, the strength recovery of the repaired panels reaches about 82 %. This higher strength
recovery indicates that the repair process conducted can restore efficiently the mechanical
performance of the damaged panels. These results are in accordance with results obtained for
the PW panels. One then can conclude that the circular patch is more efficient than the
rectangular patch. The failure mode was also different, and no buckling was observed for the
circular patch as for the 2D rectangular patch.
226
Table A-3. Compressive results of the studied configurations.
Configuration Angle
(°)
Elastic modulus
(GPa)
Failure strength
(MPa)
Strength recovery
(%)
Pristine - 40.46 376.01 100
Open-hole - 38.45 161.16 42.86
Repaired 3° 39.86 306.04 81.39
Figure A-14. Force versus strain curves of 3-circular 8HS repaired panels
Figure A-15. Force versus strain curves for 8HS open-hole honeycomb panels
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Figure A-16. Failure modes for specimens tested in compression: a. Open-hole panel,
b. 3°-repaired panel
A.3 Flexure Tests on Pristine and 2D Repaired 8HS Honeycomb
Sandwich Panels
Long-Beam Flexure Tests
Long-beam flexure tests were conducted to the 8HS pristine and repaired specimens in
accordance with the ASTM standard D7249. Specimens were tested, at room temperature
conditions, using an electromechanical MTS test frame with a100 kN load cell. A crosshead
rate of 8 mm/min was used for these tests. Strain gages, bonded in the middle of the bag and
tool facesheets, were used to measure the strain on the specimens and a fixture system as the
one used in the standard was machined, as illustrated in Figure A-17. The support span (S) and
the load span (L) were taken equal to 153 mm and 1067 mm respectively, in order to ensure
that failure occurs in the composite facesheets and to prevent core shear failure. Two main
groups of specimens were prepared to determine the flexure properties of the 8HS sandwich
beams. Namely, three pristine specimens and six 2D repaired specimens made with 5320-8HS
composite facesheets bonded with the FM300-2M adhesive film to a hexagonal Nomex
a. b.
228
honeycomb core, with a density of 96 kg/m3. The patch repair was a rectangular patch and the
studied scarf angle was 3°. Table 4 summarizes the test matrix employed for each
configuration. The failure stress was calculated using:
( )
2( )
f
f
F S L
d c Wt
(1)
where: F is the maximum recorded force during the test, c is the core thickness, d is the
measured total thickness of the sandwich panel, W is the width of the specimen and tf is the
facesheet thickness.
Figure A-17. Four-point bending fixture system
Table A-4. Test matrix for pristine and repaired specimens
Pristine specimens
3°-Repaired specimens
Repaired face in tension Repaired face in
compression
Number of
specimens 3 3 3
Dimensions (mm2) 76.2 x 1117.6 76.2 x 1117.6 76.2 x 1117.6
L
S
229
Tests Results and Interpretation
Figures A-18 to A-20 show the flexure stress-strain responses for the pristine and repaired
specimens when the repair tool facesheet is loaded in compression and in tension, respectively.
It can be seen from Figures A-18 to A-20 that the flexure response is linear until the failure
suddenly occurs. Moreover, all the observed failure modes of the tensile specimens were fiber
fracture, away from the load spans, as shown in Figures A-21 and A-22. Compressive skin
failure was observed for the pristine panel. For the repaired specimen with the repair tool loaded
in compression, the failure occurs along the scarf and the patch was entirely detached from the
panel, as illustrated in Figure A-22.a. For the repaired specimen with the repair tool loaded in
tension, the failure occurs in the parent side not too far from the scarf joint and then propagated
through the core and along the bag facesheet, as seen in Figure A-22.b.
Table 5 provides a summary of the flexure test results for the different studied configurations.
It can be observed that when the repair is loaded in tension, a higher strength recovery was
obtained in comparison with the one obtained when the repair is loaded in compression. These
results show that the 2D rectangular shape of the repair is more efficient in tension than in
compression.
Table A-5. Flexure results for 8HS sandwich panels
Configuration Angle
(°)
Deflexion
(mm)
Failure strength
(MPa)
Strength recovery
(%)
Pristine - 67.47 341.08 -
Repair in tension 3 56.25 270.34 79.26
Repair in compression 3 51.45 258 75.64
230
Figure A-18. Stress-strain curves for the 8HS pristine panels
Figure A-19. Stress-strain curves for the repaired facesheet loaded in compression
231
Figure A-20. Stress-strain curves for the repaired facesheet loaded in tension
Figure A-21. Typical failure of the pristine specimen
a. Repair in compression b. Repair in tension
Figure A-22. Failure modes for the 3°-repaired panel.
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A.4 Results Validation
The main objective of the flexure tests conducted for the 8HS skin material panels is to validate
the results obtained for the pristine and for the repaired panels under uniaxial tension and
compression loads.
Figure A-23 compares the failure stress obtained from static tensile and compression tests with
the value obtain under flexure loading for the pristine panels. It can be seen that the pristine
panels are more resistant in tension than in compression. For the flexure tests, failure occurs in
the facesheet loaded in compression. It can be observed also that the stress failure value
obtained from the compression tests is in accordance with the result obtained from the flexure
tests.
Figure A-24 compares the results for the 2D repaired panels, with a 3°-scarf angle, when the
repaired sandwich panel is loaded in flexure with the repaired facesheet either in tension or in
compression, and when it is loaded in uniaxial tension and compression. As for the pristine
panels, the value obtained for the repaired specimens from the uniaxial tension and
compression and from the flexure tests when the repair is loaded in compression or in tension
are quite similar.
233
Figure A-23. Comparison of the failure stress of the pristine panels obtained from different
loading types.
Figure A-24. Comparison of the failure stress of the 3°-repaired panels (2D repair
configuration) obtained from different loading types.
234
These results confirm that uniaxial tensile or compressive tests can be used to determine the
mechanical strength of repairs in sandwich honeycomb panels) is valid. From these results, it
is clear that the repair is quite strong when it is subjected to tensile loading applied either by
uniaxial tension and flexure.
From all the conducted tests for both the rectangular and the circular repair shapes, it is now
clear that the 3D circular repair is stronger than the 2D rectangular repair in both loading cases:
tension and compression. This may be explained by the difference in the shape and the stress
concentration in the adhesive bondline. Also, for the circular shape, the repair is surrounded by
the intact parent material however for the rectangular repair shape, the repair was along the
whole width of the panel.