Adjust Material Law to Improve Necking Behavior

In order to simulate physically the contribution of each element in the necking point, it is advisable to adjust the curve by varying the Johnson-Cook coefficients in order to increase the intensity of stress at the necking point. The main result is no longer the variation of the stress/strain curve but rather the surface under the curve which characterizes the energy dissipated during the test. This energy-based approach is relevant for crash tests since the final assessment is often more significant than how it was achieved.(1) rad_ex_fig_11-25_eq

rad_ex_fig_11-26
Figure 1. Engineering Stress/Strain Curve Obtained using Adjusted Johnson-Cook Coefficients
Figure 2 compares the new yield curve with experimental data:

ex11_fig27
Figure 2. Yield Curves
Material is described in the Johnson-Cook coefficients are (Model 3):(2) rad_ex_11-27A
Yield stress
50 [ MPa ] MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqGqFfpeea0xe9vq=Jb9 vqpeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meaabaqaciGacaGaaeqabaWaaeaaeaaakeaadaWadaqaai Gac2eacaGGqbGaaiyyaaGaay5waiaaw2faaaaa@3BE6@
Hardening parameter
350 [ MPa ] MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqGqFfpeea0xe9vq=Jb9 vqpeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meaabaqaciGacaGaaeqabaWaaeaaeaaakeaadaWadaqaai Gac2eacaGGqbGaaiyyaaGaay5waiaaw2faaaaa@3BE6@
Hardening exponent
0.38

Maximum stress is set to 189 or 190 MPa (according to the parts).

The results of adjustment to the Johnson-Cook coefficients are:

rad_ex_fig_11-28
Figure 3. Shell Contribution during the Necking Point Sequence (von Mises stress)
As the necking point progresses, more physical results are obtained due to the new input data of the material law coefficients having a better element contribution.

rad_ex_fig_11-29
Figure 4. Variation of the von Mises Stress on Elements 110, 109, 108, 107, 11 and 106

Damage Modeling with Plastic Strain Failure

The elasto-plastic model of Johnson-Cook is used until failure, which is simulated using a plastic strain failure option. The element is deleted if the plastic strain reaches a user-defined value ε max . This damage model shows good stability. A maximum plastic strain is defined for each Johnson-Cook model:

rad_ex_fig_11-30
Figure 5. ε max = 75% ; Yield Curve Close to Experimental Data: ex_11_true-strain2

rad_ex_fig_11-31
Figure 6. ε max = 47% ; Yield Curve Adjusted with Respect to Lower Stresses: ex_11_yield-curve3

rad_ex_fig_11-32
Figure 7. ε max = 40% ; Yield Curve Adjusted with Respect to High Stresses: ex_11_yield-curve4

Failure is reached for relatively high true strains.