A tensile test coupon (dog-bone) model is subjected to a dynamic tensile loading and
the results of solid and shell elements using different formulations are
evaluated.
The goal is to verify the plastic strain results by comparing them with experimental
data and Radioss results.
Model Files
Before you begin, copy the file(s) used in this problem
to your working directory.
The model represents a tensile test coupon (dog-bone model) as shown in Figure 1. The coupon is extended from one side in the X-direction, while the other side is
fixed in all six degrees of freedom using boundary conditions
(SPC). The nodes on the right-hand side of the coupon are
constrained within a rigid body definition (RBE2). A prescribed
velocity of 1m/s in the direction of extension is applied to the main node of the
rigid body (SPCD).Figure 1. Loads and Constraints
The material test data and the engineering stress-strain curves were referred from
1. Since experimental stress-strain curves are available, the tabulated material
property curve (MATS1) is selected. The formulae in Equation 1 and Equation 2 can be used to determine the true stress versus true strain curve. The plastic
part of the curve can then be isolated. This true stress vs plastic true strain
curve is used as an input of MATS1.
Where,
True strain
Engineering strain
True stress
True strain
The engineering stress can be calculated using σe = F/A0. The force is derived from
the rigid body force and the original cross-sectional area is 20.4
mm2
The engineering strain is calculated with εe = Δl/l0. The elongation Δl is measured
from two instrumented nodes. The original distance l0 is 80 mm.
Two different element formulations are used in this model and each element
formulation has been tested with two different integration types. The following
tests were conducted:
CQUAD4 Shell Elements
FULL and BWC integration types are studied
Flanagan-Belytschko Stiffness Form hourglass control is used for BWC
CHEXA Solid Elements
FULL and URI integration types are studied
Puso hourglass control is used for Uniform Reduced Integration (URI)
Material
The specimen is modeled with sheet material using MAT1, which
defines the elastic part of the stress strain curve, and MATS1,
which defines the plastic part of the curve.
Elastic-plastic Material Properties
Young's modulus
221.0
Poisson's ratio
0.3
Density
7.85E-06
Yield Stress
0.389674
Plastic Properties
Initial yield point
0.389674
TABLES1 entries for stress strain curve
Strain
Stress
0
389.6743
0.003269061
400.2301
0.006930112
409.5893
0.010444667
418.2536
0.011846377
422.4619
0.012926577
426.8274
0.013648366
433.6494
0.015225465
443.84
0.018589302
452.2541
0.02187438
469.641
0.025339483
483.1056
0.028791504
494.6843
0.032231428
505.9577
0.035658606
515.5831
0.039073858
524.8865
0.042476834
533.055
0.045868261
541.2669
0.049247692
548.5451
0.052615533
555.4787
0.055971597
561.5721
0.059316615
568.0228
0.062650303
574.1739
0.065972157
578.9182
0.069283274
584.1797
0.072583139
588.8521
0.075872187
593.5983
0.079150038
597.5798
0.082417502
602.192
0.085673728
605.6392
0.088919523
609.3784
0.092154789
613.0725
0.095379505
616.5503
0.098593692
619.6955
0.101797797
623.3059
0.104991363
626.2954
0.10817488
629.5215
0.111348321
632.8131
0.114511357
635.3597
0.117664394
637.8515
0.120807432
640.1715
0.123940737
642.7274
0.127064396
645.5801
0.130178021
647.7906
0.133282182
650.4157
0.136376459
652.4523
0.139461486
655.1424
0.142536808
657.36
0.145602624
659.3996
0.148658992
661.2593
0.151706339
663.7797
0.154744129
665.6395
0.15777259
667.1959
0.160792519
670.1453
0.163802712
671.6394
0.166804116
673.6798
0.169796749
676.2103
0.172779798
677.2082
0.175754158
678.6314
0.17871969
680.051
0.181676645
681.9008
0.184624849
683.6876
0.187564155
684.9119
0.190494822
686.0692
0.193600271
686.6066
0.196220092
687.8017
0.19941797
689.0229
Results
The analysis demonstrates the behavior of the tabulated MATS1
material’s stress-strain curve under tensile loading conditions. The simulation
results of the engineering stress-strain curves align perfectly with the
experimental data and the results from Radioss for all
element formulations and integration types. The true stress versus true strain curve
is directly extracted from an element at the center of the coupon for all the
analyses and the results are as follows:
Model with hexahedron elements CHEXA solved using Uniform Reduced Integration (URI)
with Puso hourglass control (HGTYP = 2)Figure 2. Plastic Strain Contour for Solid Element with URI Formulation and Puso HG
Control Figure 3. Comparison of Results using MATS1 for Solid Element with URI Formulation
and Puso HG Control
Model with CHEXA elements solved using full integrationFigure 4. Plastic Strain Contour for Solid Element with Full Integration Figure 5. Comparison of Results using MATS1 for Solid Element with Full
Integration
Model with CQUAD4 elements solved using Belytschko-Wong-Chiang (BWC) with
Flanagan-Belytschko stiffness form hourglass control (HGTYP =
3)Figure 6. Plastic Strain Contour for BWC Shell Formulation with Stiffness Hourglass
Control Figure 7. Comparison of Results using MATS1 for Shell BWC Formulation with
Stiffness Hourglass Control
Model with CQUAD4 elements solved using FULL integrationFigure 8. Plastic Strain Contour for Full Integration Shell Formulation Figure 9. Comparison of Results using MATS1 for Full Integration Shell
Formulation
Note: The necking begins at 0.2, so to visualize all elements with plastic strain
above this threshold, the second level of the legend is set to 0.2.
Reference
1 Li,
Wenchao & Liao, Fangfang & Zhou, Tianhua & Askes, Harm. (2016).
Ductile fracture of Q460 steel: Effects of stress triaxiality and Lode angle.
Journal of Constructional Steel Research. 123. 1-17.
10.1016/j.jcsr.2016.04.018.