Assignment 4-RADIOSS Material Laws Challenge
Assignment 4
Aim
To compare and analyze the rupture plate simulation using different material properties
Procedure
- Import the failurejohnson_000.rad file to hypermesh

Figure 1
- After this, export the file to a new folder

Figure 2
- An alternative is to simply name the file appropriately with a _0001.rad end so that radioss solver will identify it properly.
- The first case is the default simulation so simply go to analyse->radioss and run the analysis in the folder.

Figure3
- Note the input file should direct to a new folder as otherwise the files can get mixed up
- The various cases are shown in Table 1
|
Case 1 |
Run the default setup |
|
Case 2 |
Make modifications to lfail_sh=1, Dadv=1 and lxfem =2 to the fail Johnson card. Refer Figure 4 |
|
Case 3 |
Delete the /fail/johnson card and run the simulation |
|
Case4 |
Delete the value of EPS_p_max in the material aluminium card. Refer Figure 5 |
|
Case 5 |
Change the card image to law1 elastic with the same values of density, E and nu. Refer Figure 6 |
|
Case 6 |
Change the card image to law 36 with appropriate values |
|
Case 7 |
Run law27_000.rad with the recommended property values |

Figure 4

Figure 5

Figure 6
- In case 6, we make several changes to the material card.
- Firstly, we change it to law 36 Plastic Tabulated material and add the appropriate values.

Figure 7

Figure 8
- For the function id, it is necessary to create a curve according to the values given in figure 9.

Figure 9
- Go to curves, and create a new curve.

Figure 10

Figure 11
- Before we compare the graphs of the various cases, let us view the animations against each other with von mises contour enabled.

Figure 12
- At around t=4 or frame9, it can be easily observed that in case 2 the crack propagation is better defined and the stresses are more clear
- This can be attributed to the fact that in case 2, in the failure card, we set lfail_s=1, lx_fem=1 and dadv=1 which capture the animation more accurately.
- lfail Determines the Shell Element Failure Method
- lx_Fem determines whether failed elements crack or get deleted
- dadv determines how many pieces an element can break into before deletion

Figure 13
- In case3 the failure johnson card has been deleted.
- On comparing it with case 2, it can be observed that the failure of the component is more realistic in case 2 than in case 3 where the region fails uniformly.

Figure 14

Figure 15

Figure 16
- In case 4, the value of Eps_max is deleted, this defaults to a very high value so failure is not observed in this animation

Figure 17

Figure 18
- In case 5, the Material card is changed to elastic.
- It can be observed that the stress distribution and deformation is more proper in case 5 over case 4
- The maximum stress experienced in case 5 is significantly more compared to that in case 4.

Figure 19

Figure 20
- In Case 6, the material card is changed to law36 Elasto Plastic.
- On comparing with Case 5 which had an elastic material card, we can clearly observe the difference as the component fails more explosively in case 6 which is usually what is observed with brittle materials

Figure 21
- In case 7, the material card is changed to Plastic Brittle.
- The difference can clearly be observed as there is plastic deformation in case 7
- After some plastic deformation, the region fails similar to brittle materials.

Figure 22

Figure 23
- Now, let us look at the graphs of each simulation.
- Case 1:In this case we are running the default simulation with the failure johnson card and having lx_fem lfail and dadv as
- The internal energy linearly increases up to 4ms after which it becomes constant

Figure 24
- This can be attributed to the fact that after 4ms failure occurs which result in element deletion.
- The spikes in kinetic energy further confirm this as element deletion allows the ball to move freely and resulting in element vibration around the region

Figure 25

Figure 26
Simulation 2
- In this case, we modify the failure johnson card and set lfail_sh=1,dadv=2 and lx_fem=1.
- These modifications change the way failed elements react and thus enable us to properly visualize crack propagation
- This case is the most realistic scenario if the material used is aluminium.
- After around 4ms.the elements get deleted resulting in constant internal energy.

Figure 27
- The kinetic energy has a large spike after 4ms.suggesting element deletion and vibration in the region.

Figure 28
In case 3, the failure johnson card is deleted after which the simulation is run.
- Esp_max determines element failure, that is if the value of strain across any integration point crosses 15.1% of plastic strain they get deleted
- There is a linear increase in energy until a bulk of the elements get deleted
Figure 29

Figure 30
- In Case4, the Esp_Max value has been deleted.
- In this case, radioss assigns it an extremely high default value
- The material behaves like a pseudoelastic material since there are no failed elements to delete
- The kinetic energy, in this case, is negligible in comparison to the internal energy

Figure 31

Figure 32
- In case 5, the material is law1 elastic with defines the basic properties of elastic materials
- It considers only the elastic phase of the materials, there is no plasticity, resulting in Linear Deformation. This purely elastic property assigned also results in no element failure.
- The kinetic energy gradually increases as the plate is stretched
- The internal energy increases exponentially due to the elastic nature of the material
- The maximum stress experienced by the plate is significantly larger compared to previous cases due to the elastic nature of the material

Figure 33

Figure 34
Case 6
- In this case, the material exhibits strongly brittle behaviour. There is no bending and it almost immediately breaks.
- There is no significant crack formation and the stress is not dissipated across the region. It is localized around the region of impact
- There is an almost linear relation between Internal energy and time until element failure after which it becomes constant.

Figure 35

Figure 36
- In Case 7, we use Law 27 Plastic Brittle Material
- The sheet absorbs more force before failure in comparison to case 6
- The graph plateaus around the 4ms mark which coincides with element deletion

Figure 37

Figure 38
- Comparison between energy error%, mass error, element failure, no of cycles and solver time is given in table 2.
|
Case |
Time |
No of Cycles |
Mass error |
Energy Error |
Element Failure |
|
1 |
442.11 |
49380 |
0 |
0.8 |
Deleted |
|
2 |
651.67 |
49217 |
0 |
4.1 |
Elements crack before deformation |
|
3 |
456 |
49408 |
0 |
0.8 |
Deleted |
|
4 |
492.65 |
48737 |
0 |
3 |
No failure |
|
5 |
388.43 |
47969 |
0 |
1.3 |
No failure |
|
6 |
458.90 |
53143 |
0 |
-1.8 |
Deleted |
|
7 |
408.75 |
49508 |
0 |
0.8% |
Deleted |
Learning Outcomes
- Commonly Used Material Cards in Radioss
- Failure Cards
- Comparing and analysing the animations using contour
Result
The various material cards commonly used in Radioss have been explored using a crash analysis of a plate.
Some common Material Cards include
Law1 Elastic
Law 2 Plastic
Law 27 Brittle
Law 36 Elastic-Plastic Behaviour modified with user-defined functions