finite element modelling of entrance resistance for perforated … · 2018-09-11 · finite element...
TRANSCRIPT
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Finite element modelling of entrance resistance for perforated
HDPE subsurface drainage pipes
N. Gaj and Prof. C.A. MadramootooDept. of Bioresource Engineering
McGill University, Montreal07 Sept, 20181
CSBE/SCGAB Annual General Meeting and Technical ConferenceGuelph, 2018
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BackgroundSubsurface drainage materials
High density polyethylene (HDPE)has been used since the 1950s.
Benefits:Economically feasibleEasy to handle and transportMechanized installation
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Clay tiles
HDPE tubing
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Background
Drainage theories for subsurface pipe design assume pipe walls are completely porous.
Field installations have finite openings or perforations on the pipe wall, causing additional hydraulic head losses known as the entrance resistance, αe.
Previous evaluations of αe have been based on electrical analogue models and have not been adequately validated for corrugated HDPE pipes.
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From Dierickx, 1980
( )
−=
0
120
ln
2
RR
LkQ T φφπ
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Background
Theory for radial planar flow and entrance resistance
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From Dierickx, 1980
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Research objectivesTo develop general guidelines for perforation design in HDPE pipes used in agricultural land drainage.
to assess the effects of perforations on the flow towards the drainpipes.a) establish the zone of influence for quasi-radial flow convergence towards perforationsb) establish the effect of perforation shape, size, and pattern on the entrance resistance and delivery ratio (Q/Q0)
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Research objectives
to assess the effects of perforations on the local stresses in the walls of the drainpipes.
a) establish the effects from agro-traffic, embedment depth, and soil type on local stress concentration factors (λSC) around perforations
b) establish the effect of perforation shape, size, and pattern on the stresses (σc) and deformation (ΔD) in the pipe wall
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Research objectives
to establish design guidelines for perorations on HDPE drainpipes
a) generate design charts for the effective depth (de) vs. drain spacing (L) based on λSC and Q/Q0for Eastern Canada.
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Materials and Method
Numerical Simulations
and Analyses
•Computation of entrance resistance, αe
•Assessment of αe for various perforation shape, size , and pattern
Numerical Modelling
•Geometry and parameter set-up
•Finite Element mesh assessment
•Model Calibration
Sand tank experiments
•Characterizing porous medium
•Flow rate and piezometric head measurements
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Materials and Method
Porous medium characteristics
Property Value
Void ratio, e 0.44 to 0.83
Effective size, D10 0.34 mm
Coefficient of Uniformity, Cu 2.1
Specific Gravity, Gs 2.662
Max. Dry Density, γd max 15.62 kN/m3
Optimum Moisture Content, OMC 7.7%
Hydraulic Conductivity, Ksat (Kozeny-Carman model) 53.9 to 247.1 m/d
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Materials and Method
Sand tank experiments
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Rainfall simulators
Supply reservoir
Rectangular flume
Gated-outlet control chamber
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Materials and Method
Sand tank experiments
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Model PC:Plain Wall and Circular Holes
Model CC:Corrugated
Wall and Circular Holes
Model CS:Corrugated
Wall and Slits
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Materials and Method
Perforation pattern
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Materials and Method
Perforation pattern
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Materials and Method
Perforation pattern
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Materials and Method
Instrumentation and sensors
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CR23X data logger
V-notch discharge weir
(11° angle)
Piezometers (10 mm dia.)
Sonic sensor (SR 50)
Collection reservoir
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Materials and Method
Electrical analogue approach (Dierickx, 1980)
where:αe is the entrance resistance, m is the number of perforations per unit drain length, λ1 and λ2 are the smallest and largest perforation spacing respectively (m), δp is the diameter of the perforation (m).
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−−=
1
2
1
ln291.32
111λλ
λδπα
pea m
- arched boundary conditions on PC model
−−=
1
2
1
ln291.32
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1λλ
λδπ
πα
pep m
- plane boundary conditions on PC model
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Materials and Method
Numerical modelling
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Model geometry and set-up
Mesh generation for
model
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Materials and Method
Numerical modelling – mesh assessment (PC)
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Variation of model output with increasing
number of elements
Mesh quality for model PC
0.0E+00
2.0E-05
4.0E-05
6.0E-05
8.0E-05
1.0E-04
1.2E-04
1.4E-04
1.6E-04
- 50,000 100,000 150,000 200,000 250,000
Mod
el O
uput
Number of Elements
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Materials and Method
Numerical modelling – mesh assessment (CC)
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Variation of model output with increasing
number of elements
Mesh quality for model CC
0.0E+00
5.0E-06
1.0E-05
1.5E-05
2.0E-05
2.5E-05
Mod
el O
uput
Number of Elements
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Preliminary Results
Numerical modelling (Calibration -PC)
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Ks1 Ks2 Ks3 Ks4 Ks1 Ks2 Ks3 Ks4
cm m3/s 1.530E-03 1.560E-03 1.590E-03 1.620E-03 1.530E-03 1.560E-03 1.590E-03 1.620E-0340.1 1.4088E-04 1.357E-04 1.384E-04 1.410E-04 1.437E-04 5.1532E-06 2.4919E-06 1.6938E-07 2.8307E-0645.2 1.3979E-04 1.208E-04 1.232E-04 1.255E-04 1.279E-04 1.8982E-05 1.6613E-05 1.4244E-05 1.1875E-0550.1 1.0439E-04 1.065E-04 1.086E-04 1.106E-04 1.127E-04 2.0868E-06 4.1746E-06 6.2623E-06 8.3500E-0655.1 8.8603E-05 9.185E-05 9.365E-05 9.545E-05 9.725E-05 3.2462E-06 5.0471E-06 6.8481E-06 8.6490E-06
MAE 7.3669E-06 7.0816E-06 6.8809E-06 7.9262E-06
Simulated Discharge, Qs Absolute Error (AE)Measured
discharge, Qm
Hydraulic head on the
discharge pipe, Hd
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Preliminary Results
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Hd
Hydraulic head on outlet from
bottom of pipe
Q αe
cm cm m3/sPipe empty PC-0 27.375 0 2.36E-04 0.387373
1/4 full PC-0.25 30.2375 2.863 2.25E-04 0.4147011/2 full PC-0.5 33.1 5.725 2.14E-04 0.4449653/4 full PC-0.75 35.9625 8.588 2.02E-04 0.478651
Full PC-F 38.825 11.450 1.91E-04 0.516381PC-1 40.1 12.725 1.86E-04 0.534697PC-2 45.2 17.825 1.65E-04 0.619217PC-3 50.1 22.725 1.46E-04 0.722728PC-4 55.1 27.725 1.26E-04 0.861677
From Sand Tank
Experiments
Condition on outlet
Code
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Preliminary Results
Numerical modelling - convergence of streamlines - PC
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Plan view
Front view
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Preliminary Results
Numerical modelling - convergence of streamlines - CC
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Plan view
Front view
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Preliminary Results
Numerical simulations - convergence of streamlines with depth
24Front view
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Preliminary Results
Numerical simulations - convergence of streamlines with width
25Front view
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Preliminary Results
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Effects of the tank width, W and depth, de on the flow rate through a fully porous wall
0.0E+00
2.0E-04
4.0E-04
6.0E-04
8.0E-04
1.0E-03
0 50 100 150 200 250 300 350 400
Flow
rate
, Q0
(m3 /
s)
Width of tank, W (cm)
30.6 cm
50.6 cm
70.6 cm
90.6 cm
110.6 cm
Q0 = 6.44 E-04
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Preliminary Results
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Effects of the tank width, W and depth, de on the flow rate through perforations for model PC
0.0E+00
2.0E-05
4.0E-05
6.0E-05
8.0E-05
1.0E-04
1.2E-04
1.4E-04
1.6E-04
1.8E-04
2.0E-04
0 50 100 150 200 250 300 350 400
Flow
rate
, Q (m
3 /s)
Width of tank, W (cm)
30.6 cm
50.6 cm
70.6 cm
90.6 cm
110.6 cm
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Preliminary Results
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Effects of the tank width, W and depth, de on the delivery ratio, Q/Q0
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0 50 100 150 200 250 300 350 400
Del
iver
y Ra
tio, Q
/Q0
Width of tank, W (cm
30.6 cm
50.6 cm
70.6 cm
90.6 cm
110.6 cm
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Summary of FindingsEntrance resistances depend on the outlet condition of thedrainpipe.
The radial zone is not affected by the depth of theimpermeable layer.
The radial zone extends to 1.5 m laterally from the centre of thedrainpipe.
The benchmark model for Q0 comes within 0.7% error ofthe analytical solution for radial planar flow.
A delivery ratio of 0.28 was computed for the PC model
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Next steps
Continue the simulations and analyses for thecorrugated pipe models
Assess the effects of perforations on the local stressesin the pipe wall.
Amalgamate the hydraulic and structural designcomponents to develop general design guidelines forvarious field conditions in Eastern Canada.
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References
COMSOL Multiphysics. (2018). Subsurface Flow Module:User's Guide. USA: COMSOL.
Dierickx, W. (1980). Electrolytic analogue study of the effectof openings and surrounds of various permeabilities onthe performance of field drainage pipes. Doctoral thesis,Wageningen, Merelbeke, Belgium.
Skaggs, R. W. (1978). Effect of Drain Tube Opening on Water-Tabl e Drawdown. Journal of Irrigation and DrainageDivision, (ASCE), 104(IR1), 13-21.
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Questions? Thank You!
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Finite element modelling of entrance resistance for perforated HDPE subsurface drainage pipesBackgroundBackgroundBackgroundResearch objectivesResearch objectivesResearch objectivesMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodMaterials and MethodPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsPreliminary ResultsSummary of FindingsNext stepsReferencesQuestions? Thank You!