A snap-through problem is studied on a shallow cylindrical roof upon which an imposed velocity is applied at its mid-point.
The characteristic curve, caused by the limit load and achieved by simulation is compared to a reference. This example
is considered a static problem.
The fluid-structure interaction and the fluid flow are studied in cases of a fuel tank sloshing and overturning. A
bi-phase liquid-gas material with an ALE formulation is used to define the interaction between water and air in the
fuel tank.
The impact and rebound between balls on a small billiard table is studied. This example deals with the problem of
defining interfaces and transmitting momentum between the balls.
Apart from the experimental results, the modeling of the strain rate effect on stress will be considered at the end
of this example using a sensitivity study on a set of parameters for Johnson-Cook's model.
The Johnson-Cook model previously defined corresponds to the experimental results up to the necking point. However,
the slope of the numerical response does not enable the necking point to start at the strain value observed experimentally.
LAW27 is used to simulate material damage following a Johnson-Cook plasticity law. Thus, model damage is associated
with the previous law in order to take account of failure.
This is a tabulated law; therefore, the true stress versus plastic strain function can be directly used. The rupture
phase can be simulated by adding points to this hardening function.
After a quasi-static pre-loading using gravity, a dummy cyclist rides along a plane, then jumps down onto a lower
plane. Sensors are used to simulate the scenario in terms of time.
The transitory response of a perfect gas in a long tube separated into two parts using a diaphragm is studied. The
problem is well-known as the Riemann problem. The numerical results based on the SPH method and the finite element
method with the Lagrangian and Eulerian formulations, are compared to the analytical solution.
This example compares different studies with flexible or rigid bodies. The method for using the flexible bodies in
an explicit analysis is also studied.
The problem of a dummy positioning on the seat before a crash analysis is the quasi-static loading which can be resolved
by either Radioss explicit or Radioss implicit solvers.
The crashing of a box beam against a rigid wall is a typical and famous example of simulation in dynamic transient
problems. The purpose for this example is to study the mesh influence on simulation results when several kinds of
shell elements are used.
A square plane subjected to in-plane and out-of-plane static loading is a simple element test. It allows you to highlight
element formulation for elastic and elasto-plastic cases. The under-integrated quadrilateral shells are compared with
the fully-integrated BATOZ shells. The triangles are also studied.
The modeling of a camshaft, which takes the engine's rotary motion and translates it into linear motion for operating
the intake and exhaust valves, is studied.
The ditching of an object into a pool of water is studied using SPH and ALE approaches. The simulation results are
compared to the experimental data and to the analytical results.
An explicit stamping simulation is followed by a spring-back analysis using implicit or explicit solvers for stress relaxation.
Results are compared with a reference.
A cantilever beam submitted to a shear-bending is tested by Radioss linear and nonlinear solvers. Different kinds of Radioss finite elements provide results close to the analytical one.
A rubber ring resting on a flat rigid surface is pushed down by a circular roller to produce self-contact on the inside
surface of the ring. Then the roller is simultaneously rolled and translated so that crushed ring rolls along the
flat surface.
Polynomial EOS is used to model perfect gas. Pressure or energy can be absolute values or relative. Material LAW6
(/MAT/HYDRO) is used to build material cards for each of these cases.
Separate the whole model into master domain and sub-domain and solve each one with its own timestep. The new Multi-Domain
Single Input Format makes the sub-domain part definition with the /SUBDOMAIN keyword.
The Cylinder Expansion Test is an experimental test used to characterize the adiabatic expansion of detonation products.
It allows determining JWL EOS parameters.
The purpose of this example is to compare the simulation results to experimental data. Radioss includes the material model CONC to model concrete failure modeling under compression and tension.
A container that is partially filled with liquid is dropped and the interaction between the liquid and structure can
be studied. The liquid fill is defined using /INIVOL and infinite plane /SURF/PLANE. The contact between the structure and liquid is defined using /INTER/TYPE18.
A heat source moved on one plate. Heat exchanged between a heatsource and a plate through contact, also between a
plate and theatmosphere (water) through convective flux.
The target of cut methodology is to study one area of the model with taking into account the deformation of the full model
through a section force. In the defined section, displacement will be imposed in order to represent the "sub" part of
the model. This cut methodology is used to save the computation time. It is often used for component structure study.
The aim of this example is to show how to use /SECT to apply this technique.
Impacts of rotating structures usually happen while the structure is rotating at a steady state. When the structure is
rotating at very high speeds, it is necessary to include the centrifugal force field acting on the structure to correctly
account for the initial stresses in the structure due to rotation.
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)
Figure 1. Engineering Stress/Strain Curve Obtained using Adjusted Johnson-Cook
Coefficients
Figure 2 compares the new yield curve with
experimental data: Figure 2. Yield Curves
Material is described in the Johnson-Cook coefficients are (Model 3):(2)
Yield stress
50
Hardening parameter
350
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: 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. 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 . This damage model shows good stability. A maximum plastic
strain is defined for each Johnson-Cook model: Figure 5. = 75% ; Yield Curve Close to Experimental Data:
Figure 6. = 47% ; Yield Curve Adjusted with Respect to Lower
Stresses: Figure 7. = 40% ; Yield Curve Adjusted with Respect to High
Stresses:
Failure is reached for relatively high true strains.