lecture 9 nlfm ctoa

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  • 7/28/2019 Lecture 9 Nlfm Ctoa

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    CEE 770 Meetings 9 and 10

    Objectives of These Meetings

    Introduce Issues and Approaches for

    Non-Linear Fracture Mechanics (NLFM)

    What makes NLFM more difficult than LEFM?

    NLFM Approaches under Development

    A NLFM Approach for Thin Metallics: CTOAc (Meeting 9)

    A NLFM Approach for Many Other Situations:

    Cohesive Fracture Mechanics (Meeting 10)

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    What makes NLFM more difficult than LEFM?

    1. The Process Zone is too large relative to the crack length:

    Therefore, SIFs lose their meaning, and value. We no longer have a

    single parameter that completely controls all action in the process zone.

    We now have to solve a local, materially non-linear problem, and wemust expect that similar structural geometries and BCs will produce dis-

    similar locally non-linear results. Therefore, toughness for a given

    material is no longer a material state value.

    rpa

    183

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    What makes NLFM more difficult than LEFM?

    2. The Process Zone might be too large relative to other structural dimensions:The problem is now one of full (structural) scale inelasticity, and we can

    expect conditions for crack growth to be very sensitive (more so than in case

    1.) to changes in geometry and/or BCs.

    Again, theoretically we would have to:

    a. Compute local fields from non-linear

    analysis, and

    b. Measure resistance to crack extension

    case-by-case!

    What simplifications can we get away with?

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    NLFM Approaches under Development

    Since the late 1960s, many NLFM theories and approaches have been

    proposed. All are of limited use. Few have any standardized testing or

    computational methodologies associated with them.

    For material states characterized by elasto-plastic process zone behavior,

    the crack tip opening displacement (CTOD) and the EP J-Integral have seen

    most development and use. (Read Chapter 3 of Anderson!).

    For many other non-linear material states, the so-called cohesive fracturemechanics approach is seeing rapid development and use. (Not in

    Anderson!).

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    CEE 770 Meeting 9

    Objectives of This Meeting

    Learn the CTOAc concept for some types of NLFM problems:

    Steady-state plastic zone evolution, and stable tearing

    EP FEM methods for calibrating and then predicting

    Example applications

    Using FRAN2D/L and the CTOAc criterion.

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    A Common NLFM Problem Involves EP

    Crack Growth in Thin Sheet Structures

    Like Aircraft FuselagesShip Hulls???187

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    Features of Stable Crack Growth Under

    NLFM Conditions

    Active plastic zone

    Residual plastic strain from

    elastic unloading

    Envelope of previous

    plastic zones

    Elastic-plastic

    If this process can reach a steady-state before global (structural scale) crack

    instability, maybe we can find a local feature to measure, and then compute

    and use as a stable crack growth criterion. One possible feature is the CTOA.

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    Crack Tip Opening Angle (CTOA) Fracture Criterion

    d

    CTOAc

    CTOD

    Optical microscopy

    Digital image correlation

    CTOAc

    (degrees)

    a (mm)

    2.3 mm thick (B)

    2024 aluminum alloy

    When the CTOA at a specific distance,d, from the crack tip reaches a critical

    value, the crack can grow:

    Foil test

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    3-D EP Finite Element Analyses Can Be Performed to Find a

    Critical CTOA Value that Best Fits the Results of One Test

    a

    W

    C(T)

    Dawicke and Newman, Residual strength predictions for multiple site damage cracking using a three-dimensional finite element

    analysis and a CTOA criterion, Fatigue and Fracture Mechanics: 29th Volume, ASTM STP 1332, Panontin and Sheppard Eds., 1999190

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    This CTOAc Value Can Then Be Used to Predict the

    Failure Load for Structures of Different Sizes and Shapes

    191

    a

    W

    C(T)

    2a

    W

    M(T)

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    The Critical CTOA

    Must Be Calibrated

    for:

    Material Thickness

    Distance behind the

    crack-tip where it ismeasured

    Convergence studies show that the

    predicted failure load is relatively

    insensitive to near-tip element sizes,provided that there is at least one

    node between the crack tip and the

    node where the CTOAc is measured.

    Once calibrated, the CTOAc can be

    used to predict the failure load instructures of a different size or with

    different structural details.

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    0 10 20 30 40 50

    50

    100

    150

    200

    250

    0 5 10 15

    50

    100

    150

    200

    250

    0 5 10 15 20 25

    50

    100

    150

    200

    250

    Experimental Measurements

    Numerical Predictions

    applied stress (MPa)

    half crack extension, a (mm)

    applied stress (MPa)

    half crack extension, a (mm)

    half crack extension, a (mm)

    applied stress (MPa)

    0 20 40 60 80 100

    50

    100

    150

    200

    250

    half crack extension, a (mm)

    applied stress (MPa)

    w = 76 mm (3 in.) w = 305 mm (12 in.)

    w = 610 mm (24 in.) w = 1524 mm (60 in.)

    Similar Analyses Can Be Performed Using Thin-Shell,

    EP Finite Elements

    w2

    d = 0.04"

    CTOA

    Chen, Wawrzynek, and Ingraffea, Elastic-plastic crack growth simulation and residual strength predictions of thin plates

    with single and multiple cracks, Fatigue and Fracture Mechanics: 29th Volume, ASTM STP 1332, Panontin and

    Sheppard Eds., 1999 193

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    Calibration with Tests 2024_FAA_TL3 & TL4

    to determine critical CTOA on Thin Plate24

    40

    0 0.5 1 1.5 2 2.5 3

    10

    20

    30

    Half Crack Extension (inches)

    4.04.55.05.5

    Applied

    Stress

    (ksi)

    one half plane-

    strain core

    heights0.04

    194

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    KC-135 Crack Configuration

    Analyses performed under USAF Contract No. F9603-97-C-0349, Subcontract NCI-USAF-9128-001, Corrosion Damage Assessment Framework 195

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    A Recent KC-135 Failure

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    Plastic Zone Evolution and Stable Tearing in KC-135 Fuselage Panel

    Under CTOAc Criterion

    508 mm

    254 mm

    Effective Stress (ksi)

    60

    39

    53

    46

    Yield

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    Predicted KC-135 Residual Strength

    (initial lead crack length = 10.0 inches)

    Total Crack Extension (inches)0 1 2 3 4

    2

    4

    6

    8

    10

    12

    14

    16No MSD (RS = 15.3 psi)

    MSD = 0.025 in. (RS = 11.3 psi)

    MSD = 0.025 in., Corrosion (RS = 10.8 psi)

    required residual strength (12.5 psi)

    Pressure

    (psi)

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    7.14 or 10 in.

    20 in.

    Corrosion thinningMSD

    Lead crack

    12 DamageConfigurations

    Lead crack--7.14 or 10 in.

    MSD--0.025 in. or 0.046 in.

    symmetric about and at three rivets in front

    of lead crack

    emanating from both sides of a rivet hole Corrosion--10% material thinning

    uniform reduction in thickness of the upperskin199

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    Predicted residual strength: summary

    12.5

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    Plane stress or thin shell analyses can accurately predict residual

    strengths with the use of a plane strain core

    plane stress

    elements

    3-D analyses show that, in the crack-tip region, the through-the-

    thickness behavior is more similar to plane strain than to plane

    stress.

    Plane strain

    core height

    plate thickness

    plane strain elements

    Plane strain (or special thin shell elements) are placed in a small

    region or strip along the crack path.

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    Failure Load Predictions for Analyses Using

    a Plane-Strain Core (PSC)

    Dawicke, Residual strength predictions using a crack tip opening angle criterion, Proc. Of the FAA-NASA symposiumon the continued airworthiness of aircraft structures, Atlanta, GA, 1997

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