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OBJECTIVE: To model a set of spot welds for the given assembly of parts by using both 1d beam elements and 3d Hexa elements. To simulate a crash test for the given assembly and compare the results in both the cases. Deliverables ==> - Input .k file and output files (d3plot, glstat, sleout, rcforc)…
Kiran Ks
updated on 18 Sep 2020
OBJECTIVE:
Deliverables ==> | |
- Input .k file and output files (d3plot, glstat, sleout, rcforc)
- Animation of the final simulation
- The cross-sectional force generated in the middle of the crash box (along its length)
- Acceleration plot of a node in the middle of the crash box (along its length)
- Maximum directional stress and strain along the length of the crash box (X strain, Y strain, etc)
- A plot of all energies (total, internal, kinetic, hourglass, sliding)
- Compare the results
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PROCEDURE:
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Fig. 1. The imported keyword file
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Fig. 2. The material and section cards assigned to the two parts
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Fig. 3. Beam elements(8nos) created to model the spot welds
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Fig. 4. Material and section cards for the beams representing the spot welds.
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Fig. 5. Contact cards defined for the crash
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Fig. 6. A rigid wall created and initial velocity applied to the parts
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Fig. 7. Setting the simulation runtime using the *CONTROL_TERMINATION card |
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(i) | (ii) |
Fig. 8(i) Case 1(Using 1d beam elements); (ii) Case 2(Using 3d Hexa elements)
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Fig. 9. Output requests made using the ASCII card
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Fig. 10. The *DATABASE_CROSS_SECTION_PLANE_ID and *DATABASE_HISTORY_NODE cards
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Fig. 11. The *DATABASE_BINARY_D3PLOT card
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RESULTS & DISCUSSION:
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(i) Case 1 | (ii) Case 2 |
Fig. 12. Crash animation
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The crash animation shows the assembly crashing against the rigid wall at ~ 1 ms. All the spot welds fail at exactly 2.5 ms in both cases. In both cases, on impact against the wall, the bottom bracket tends to bounce back. This rebound motion of the bottom bracket is transferred to the top bracket via the spot welds. After the failure of the spot welds at 2.5 ms, the top bracket is no longer restrained by the bottom bracket and begins to freely move ahead with its inertia. While in case 1, the bottom bracket can be seen to have come to nearly zero rebound velocity due to the inertia effect of the top bracket, in case 2, the assembly appears to be stiffer and there is almost zero rebound, possibly due to higher inertia of the whole assembly arising from the use of solid elements to represent the welds. |
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(i) Case 1 | (ii) Case 2 |
Fig. 13. Stress contour
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Stress contour shows the stresses getting developed on the two brackets as the crash takes place. A greater amount of stress seems to have transferred to the top bracket in case 2. Red regions signifying stress concentration are present near the spot weld regions in case 2. This may be because of a greater stiffness value for the spot welds modeled using solid elements. |
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(i) Case 1 | (ii) Case 2 |
Fig. 14. Plastic strain contour
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The maximum strain recorded were 0.00384 and 0.0047 for case 1 and 2 respectively. The region around the spot welds can be seen to have gotten strained in case 2 whereas nothing like that is observed in case 1. |
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(i) Case 1 | (ii) Case 2 |
Fig. 15. Stress-strain plots
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The figure shows the stress-strain plot generated by using the stress and strain values recorded on element number 106880. The stress-strain plots for both cases are identical. The material defined for the model has a yield stress of 250 MPa. Here, the maximum stresses observed are 136 MPa and 167 MPa for cases 1 and 2 respectively. |
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(i) Case 1 | (ii) Case 2 |
Fig. 16. Stress plots
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The stresses recorded of element number 106880 was plotted against run time to obtain the stress plots shown in the above figure. The plots show a higher amount of stress being recorded in case 2 compared to case 1. The maximum stresses are 137 MPa and 167 MPa for cases 1 and 2 respectively. |
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(i) Case 1 | (ii) Case 2 |
Fig. 17. Strain plots
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The strain plots were also generated from the values recorded for element number 106880. The two plots are very identical with not much difference. |
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(i) Case 1 | (ii) Case 2 |
Fig. 18. Global energy plots
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The global energy plots are as expected. The total energy remained constant throughout the simulation while the kinetic and internal energies kept on changing as the crash happened. Kinetic energy can be seen decreasing at ~ 1ms when the impact takes place. This decrease in Kinetic energy is reflected as a corresponding increase in Internal energy. The Internal energy reaches a peak when the bottom bracket is at the verge of rebounding and it then decreases as the bracket rebounds with some velocity. Again due to the inertia factor of the top bracket, this rebound velocity decreases, which explains the increase in the internal energy at ~1.2 ms before finally coming to a constant value close to 80 N-m in case 1. This value is much higher(92 N-m) for case 2. |
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(i) Case 1 | (ii) Case 2 |
Fig. 19. Acceleration plots
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The acceleration plots were generated from the history data of node number 508406 in both cases. The plots are identical. The Max acceleration recorded is 1600 mm(ms)2 and 1510 mm(ms)2 for cases 1 and 2 respectively. |
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(i) Case 1 | (ii) Case 2 |
Fig. 20. Velocity plots
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The velocity plot shows a uniform velocity of 10 mmms until the impact and thereafter, the velocity decreases and goes to a negative value and finally becomes nearly zero as the simulation progresses. However, in case 2, after rebounding, the bracket has again achieved a positive velocity owing to a higher inertia factor in this case. |
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(i) Case 1 | (ii) Case 2 |
Fig. 21. Sectional forces plot
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The above plot shows the resultant force recorded on a section created on the top bracket just after the weld regions. The graphs show that a higher amount of force has been transferred to the top bracket in case 2. The max force recorded in case 2 is 14200 N whereas the same recorded for case 1 is only 3130 N. This can be a result of the Hexa elements being used to model spot welds in case 2. |
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(i) Case 1 | (ii) Case 2 |
Fig. 22. Spot weld Resultant forces
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The max resultant force for case 1 is 466 N and for case 2 is 1950 N. |
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(i) Case 1 | (ii) Case 2 |
Fig. 23. Spot weld axial force
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Axial forces recorded for case 2 are significantly higher compared to the ones recorded for case 1. This further implies the increased stiffness in the case of Hexa elements. |
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(i) Case 1 | (ii) Case 2 |
Fig. 24. Spot weld shear force
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Shear forces on the weld elements in case 1 are significantly lower compared to the values for case 2. The max shear force recorded for case 1 is 276 N whereas the same recorded in case 2 is 1890 N. |
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(i) Case 1 | (ii) Case 2 |
Fig. 25. Spot weld length
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The spot welds modeled using 1d beam elements undergo elongation on the application of force, whereas the ones modeled using Hexa elements don't undergo any elongation. This is clearly observed from the above graph. |
Max-Stress(MPa) | Max-Strain | |||||
Case | X-Direction | Y-Direction | Z-Direction | X-Direction | Y-Direction | Z-Direction |
1 |
267.2 on Ele 108672 |
218.9 on Ele 106963 | 189.9 on Ele 109915 | 0.00119 on Ele 108672 | 0.00105 on Ele 108321 | 0.00093 on Ele 109915 |
2 | 325.4 on Ele 109958 | 278.7 on Ele 107683 | 264.2 on Ele 105331 | 0.00138 on Ele 104299 | 0.00125 on Ele 107630 |
0.00119 on Ele 105331 |
CONCLUSION:
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