It is possible to make static analysis; there is no special limitation in using RADIOSS options for running a quasi-static analysis.

In order to converge to a non-oscillating solution, one has to use a very progressive and smooth enough loading.

There are also specific options which can be used in the Runname_0001.rad file:

The material density can be artificially increased in order to increase the time step or the option /DT/NODA/CST can be used. In such a case, it is important to check that the kinetic energy remains negligible in the energy balance.

It is also recommended to use QEPH shells instead of Belytschko for this kind of analysis, since they are more accurate.

This is a low pass filter. For filtering frequencies higher than a certain frequency (which corresponds to the period T given in option /DYREL), the computation must be ran during a time greater than T.

It is possible to proceed the following way:

•	Choose in order to filter the highest frequencies of the system (a short run is sufficient). This allows to better identify the following frequencies (that is to say, the highest frequencies in the remaining signal).

Reference Metrics will not work correctly if initial stresses are too high. It is recommended to check the stress level by post-processing the Animation at time t=0.

RADIOSS Starter generates initial stresses by following the same law; which is used by the fabric (Law 19) from the reference geometry (defined in the reference file) to the initial geometry (defined in Runname_0000.rad).

Since the fabric’s behavior is elastic, the initial stresses will relax at the beginning of the computation in RADIOSS Engine, and the fabric will come back quickly to the shape it gets in the reference geometry.

If these initial stresses are too high, this process is not smooth enough and the interfaces are too excited.

So the initial size of the elements must be lower than their reference size, and a reduction factor in compression will be used in the corresponding law 19.

This reduction factor allows representing the low resistance in compression of the fabric, and also allows in case of Reference Metrics to get lower initial stresses and then a smoother deployment.

On the other hand, in case the elements are in tension in some direction with respect to their reference geometry, the initial stress level is generally too high.

It is also recommended not to deform the elements in hourglass in their initial geometry with respect to their reference geometry, since hourglass modes are not taken into account by Reference Metrics.

Advising against folding an element along its diagonal

There are three condition types in /SPH/INOUT:

General Inlet (Ityp=1):

The particles are created according to the specified mass flux through the inlet surface (defined by the density and the velocities of the particles), but particles can be created only if there are available ones. Available particles are the remaining particles in the reserve and also the ones deactivated by the outlet. If the inlet runs out of particles the computation stops.

General Outlet (Ityp=2):

The deactivated particles are the ones that have crossed the outlet surface and that have lost interaction with non-outgoing particles (particles that have not crossed the outlet surface). It means that the particles are deactivated at a certain distance of the outlet surface defined by the position of the particles and by the smoothing length less comprised between h and 2h. This distance has nothing to do with the parameter DIST. DIST is used to define the outgoing particles where the pressure is controlled, but it is recommended to use a value of DIST high enough to be sure that all outgoing particles are controlled.

Non-Reflective Frontiers (NRF) (Ityp=3):

Non-Reflective Frontiers is very similar to outlet. The main difference between these two options is the pressure. With Outlet a uniform pressure is imposed on outside particles, it is used to simulate a pressure discontinuity between inside and outside. The non-reflective frontiers is used to simulate the presence of a semi-infinite domain with a continuous evolution of the pressure between the outlet surface and the far field. Pressure in the far field is defined by fct_IDp and FscaleP. Non-Reflective Frontiers also prevents wave reflection on the outlet surface.

The /KEREL option (Kinetic energy relaxation) sets the nodal velocities to zero each time when the maximum kinetic energy is reached. The kinematic relaxation behavior is like a low-pass filter, it filters initial lower frequencies. When it filters the highest frequency, computation will then diverge. In this case, the model will need to be improved. For example, using a smaller time step may solve this kind of instability issue.

If there is no part defined in the model, then RADIOSS will give following warning message in Starter and at the end Starter stopped with error of “ABNORMAL END”.

"WARNING ID :         1114

** WARNING WHILE READING

DESCRIPTION :

  THERE IS NO DEFINED PART IN INPUT FILE.”

Or, if elements are used in model but not defined in part, then Starter will also stop with error of “ABNORMAL END”.

Please make sure all elements used in model define part. Below is an example of the typical RADIOSS model assembling: