u2.06.13 General tips for using the DYNA_NON_LINE operator#
Summary:
This document introduces the use of transient resolution methods (implicit or explicit) for the numerical simulation of nonlinear dynamic problems on a physical basis.
The general reference operator for this type of calculation is called DYNA_NON_LINE and its correct use will be facilitated by compliance with a few rules of good practice described in this document.
These usage tips cover:
- the correct definition of the model in a dynamic sense (including the initial conditions and
limits),
- the definition of discretization including the choice of the time scheme
([R5.05.05], and also see Bibliography),
the choice of amortization models,
some post-treatment tips.
Given the great diversity of non-linear problems, the user will be able to very usefully complete your reading with other more specific references:
[U2.06.03]: on amortization modeling,
[U2.06.05]: for soil-structure interaction (linear and non-linear),
- [U2.06.09]: for single and multi-support in seismic calculation of equipment
in particular,
[U2.06.10]: on the specificities of studies such as civil engineering under seismic loading,
[U2.06.11]: for the use of fluid-structure models coupled with DYNA_NON_LINE,
[U2.04.07]: use of DYNA_NON_LINE to solve slowly evolving but highly non-linear problems that have difficulty converging with STAT_NON_LINE (see bibliography),
[U2.07.04]: for the non-linear transient dynamics of a model partially reduced by dynamic condensation with DYNA_NON_LINE,
[U2.06.32]: for modeling rotating machines.
Reading the documentation [U2.04.01], which gives advice on how to use the STAT_NON_LINE operator, is also highly recommended because here you will especially deepen the specificities related to dynamics. All the aspects common to STAT_NON_LINE and DYNA_NON_LINE and which are detailed in the documentation [U2.04.01], such as the choice of parameters for the Newton algorithm, remain valid in dynamics and are therefore not included here.