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17.2 - Transitions

17.2 - Transitions

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17.2 - Transitions

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Title

Box Beam - Transitions

ex_27.2

Number

17.2

Brief Description

A steel box beam, fixed at one end, impacted at the other end by an infinite mass.

Results for meshes with different transitions are compared.

Keywords

Q4 shells
Type 7 and 11 interface
Global plasticity, iterative plasticity, and variable thickness
BT_TYPE1-3-4, QEPH, BATOZ, DKT18 and C0 formulation

RADIOSS Options

Boundary conditions (/BCS)
Rigid wall (/RWALL)
Imposed velocity (/IMPVEL)
Rigid body (/RBODY)

Input File

Mesh 0: <install_directory>/demos/hwsolvers/radioss/17_BoxBeam/Transition_mesh/mesh0/...//BOXBEAM*

Mesh 1: <install_directory>/demos/hwsolvers/radioss/17_BoxBeam/Transition_mesh/mesh1/...//BOXBEAM*

Mesh 2: <install_directory>/demos/hwsolvers/radioss/17_BoxBeam/Transition_mesh/mesh2/...//BOXBEAM*

Mesh 3: <install_directory>/demos/hwsolvers/radioss/17_BoxBeam/Transition_mesh/mesh3/...//BOXBEAM*

Technical / Theoretical Level

Advanced

Overview


Physical Problem Description

A steel box beam fixed at one end, is impacted at the other end by an infinite mass. The dimensions of the box beam are 203 mm x 50.8 mm x 38.1 mm, and its thickness is 0.914 mm. As symmetry is taken into account, only one quarter of the structure is modeled. Four kinds of mesh and three plasticity formulations are compared (global plasticity, five integration points and iterative plasticity).

Units:  mm, ms, g, N, MPa

The material used follows an isotropic elasto-plastic material (/MAT/LAW2) with the Johnson-Cook plasticity model, having the following characteristics:

Initial density: 7.8 x10-3 g/mm3
Young modulus: 210000 MPa
Poisson ratio: 0.3
Yield stress: 206 MPa
Hardening parameter: 450 MPa
Hardening exponent: 0.5
Maximum stress: 340 MPa

 

fig_17-1

Fig 26: Problem studied

Analysis, Assumptions and Modeling Description


Modeling Methodology

Four types of mesh are used to model the beam. The beam is divided into two parts: a fine mesh for one half (8 x 26 elements) and a coarse mesh for the other half. Transition between the two meshes of a single beam is carried out using a mesh transition element of the same length as each particular case. You will compare results using a reference case which has a uniform mesh.

The layout of the elements is shown in the following diagram.  The following are tested for each model:

1.Element formulation:
BT_TYPE1
BT_TYPE3
QEPH
BATOZ
C0
DKT18
2.Plasticity:
Global plasticity
Progressive plasticity with five integration points
Iterative plasticity with five integration points and variable thickness

fig_17-27

Fig 27: Meshes

RADIOSS Options Used

Boundary conditions:

Take into account the symmetry, all nodes in the Y-Z plan are fixed in a Y translation and an X and Z rotation. One quarter of the structure is modeled.

Rigid body:

The lower (fixed) end is modeled using a rigid body connecting all lower nodes (Z = 0.0). The rigid body is completely fixed in translations and rotations.

Wall:

The impactor is modeled by a sliding rigid wall using a fixed velocity (13.3 m/s) in the Z-direction and fixed for other translations and rotations.

Interfaces:

The structure’s self-impact is modeled using a type 7 interface on the full structure. The interface master surface is defined using the complete model. The slave nodes group is defined using the master surface.

On top of the beam, the possible edge-to-edge impacts are dealt with using a type 11 self-impacting interface. The edges use the master surface of the type 7 interface as the input surface.

fig_17-28

Fig 28: Boundary conditions.

Simulation Results and Conclusions


The results are compared using three different views:

Role and influence of the mesh for a given type of element formulation
Shell element formulations for a given mesh
Plasticity options for a given mesh and element formulation

Three criteria are used to compare the quality of the results obtained:

Crushing force versus displacement

The crushing force corresponds to the normal force in the Z-direction of the impactor (rigid wall), multiplied by 4 due to symmetry.

For comparison, displacement corresponds to the Z-direction motion of the rigid wall’s master node.

Hourglass energy
Total energy

Total energy is the sum of all energies.

Mesh Influence for a Given Shell Using Global Plasticity

BATOZ

fig_17-29

Fig 29: Total energy for a BATOZ formulation.

fig_17-30

Fig 30: Force for a BATOZ formulation.

QEPH

fig_17-31

Fig 31: Total energy for a QEPH formulation.

fig_17-32

Fig 32: Force for a QEPH formulation.

BT_TYPE1

fig_17-33

Fig 33: Total energy for a BT_TYPE1 formulation.

fig_17-34

Fig 34: Hourglass energy for a BT_TYPE1 formulation.

fig_17-35

Fig 35: Force for a BT_TYPE1 formulation.

BT_TYPE3

fig_17-36

Fig 36: Total energy for a BT_TYPE3 formulation.

fig_17-37

Fig 37: Hourglass energy for a BT_TYPE3 formulation.

fig_17-38

Fig 38: Force for a BT_TYPE3 formulation.

BT_TYPE4

fig_17-39

Fig 39: Total energy for a BT_TYPE4 formulation.

fig_17-40

Fig 40: Hourglass energy for a BT_TYPE4 formulation.

fig_17-41

Fig 41: Force for a BT_TYPE4 formulation.

C0

fig_17-42

Fig 42: Total energy for a CO formulation.

fig_17-43

Fig 43: Force for a CO formulation.

DKT18

fig_17-44

Fig 44: Total energy for a DKT formulation.

fig_17-45

Fig 45: Force for a DKT formulation.

Influence of Element Formulation Using Mesh 3 and Global Plasticity

fig_17-46

Fig 46: Total energy for different element formulations.

fig_17-47

Fig 47: Total energy for different element formulations.

fig_17-48

Fig 48: Hourglass energy for different element formulations.

fig_17-49

Fig 49: Force for different element formulations.

fig_17-50

Fig 50: Displacements for different element formulations.

Influence of Plasticity Options Using Mesh 1 and BT_TYPE3 Formulation

fig_17-51

Fig 51: Total energy for different plasticity computations.

fig_17-52

Fig 52: Hourglass energy for different plasticity computations.

fig_17-53

Fig 53: Force for different plasticity computations.

MESH 0

ex_17_mesh_00

MESH 1

ex_17_mesh_1-1

MESH 2

ex_17_mesh_2-2

MESH 3

ex_17_mesh_3-3

ex_17_mesh_qeph

Formulation:  QEPH

ex_17_mesh_bt_type1

Formulation:   BT_TYPE1

ex_17_mesh_bt_type3

Formulation:  BT_TYPE3

ex_17_mesh_bt_type4

Formulation:  BT_TYPE4

ex_17_mesh_co

Formulation:  C0

ex_17_mesh_dkt18

Formulation: DKT18

ex_17_mesh

ex_17_table

ex_17_table2