Difference between revisions of "Examples"

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The following examples are provided to illustrate how users could use FEAP to solve some basic problems.
The following alphabetical list of examples are provided to illustrate how users could use FEAP to solve some basic problems.


== Static Analyses ==
== Contact Problems ==
A simple 2D example of a [[deformable indenter]] being pushed into a block of material


== Thermal Analyses ==
== Coupled Thermo-mechanical Analyses ==
Example of a [[hollow thermal tube]] with external temperatures and inner fluxes
 
Example of a [[3D hollow thermal tube]] with external temperatures and inner fluxes


== Coupled Thermo-mechanical Analyses ==
== Buckling: Branch Switching ==
It is possible to [[Branch Switch]] in FEAP when using the arclength method.


== Hill-Mandel Computations ==
== Hill-Mandel Computations ==
FEAP has a facility for computing [[Hill-Mandel]] averages, stress and tangent tensor components.
FEAP has a facility for computing [[Hill-Mandel]] averages, stress and tangent tensor components.
To use this facility one needs to have a periodic mesh.
To use this facility one needs to have a periodic mesh.
== Lysmer-Kuhlmeyer boundary conditions ==
FEAP has a simple [[Lysmer-Kuhlmeyer]] boundary element that can be used to approximate a non-reflecting
boundary in a transient computation.
== Contact Problems ==


== Isogeometric Analyses ==
== Isogeometric Analyses ==
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feature is slightly experimental so please verify that you are getting sensible
feature is slightly experimental so please verify that you are getting sensible
answers for your class of problems before relying on it.
answers for your class of problems before relying on it.
== Lysmer-Kuhlemeyer boundary conditions ==
FEAP has a simple [[Lysmer-Kuhlemeyer]] boundary element that can be used to approximate a non-reflecting
boundary in a transient computation.
== Plate buckling ==
[[Plate buckling]] and shell buckling computations came be made using FEAP's linear shell element.
== Spin boundary condition ==
A [[Spin boundary]] condition is possible via the use of the SPIN command within a LOAD GROUp
== Static Analyses ==
== Thermal Analyses ==
Example of a [[hollow thermal tube]] with external temperatures and inner fluxes
Example of a [[3D hollow thermal tube]] with external temperatures and inner fluxes

Latest revision as of 17:48, 31 May 2024

The following alphabetical list of examples are provided to illustrate how users could use FEAP to solve some basic problems.

Contact Problems

A simple 2D example of a deformable indenter being pushed into a block of material

Coupled Thermo-mechanical Analyses

Buckling: Branch Switching

It is possible to Branch Switch in FEAP when using the arclength method.

Hill-Mandel Computations

FEAP has a facility for computing Hill-Mandel averages, stress and tangent tensor components. To use this facility one needs to have a periodic mesh.

Isogeometric Analyses

J-Integral Computation

FEAP has a facility for computing J Integrals (energy release rates) in elastic problems. The feature is slightly experimental so please verify that you are getting sensible answers for your class of problems before relying on it.

Lysmer-Kuhlemeyer boundary conditions

FEAP has a simple Lysmer-Kuhlemeyer boundary element that can be used to approximate a non-reflecting boundary in a transient computation.

Plate buckling

Plate buckling and shell buckling computations came be made using FEAP's linear shell element.

Spin boundary condition

A Spin boundary condition is possible via the use of the SPIN command within a LOAD GROUp

Static Analyses

Thermal Analyses

Example of a hollow thermal tube with external temperatures and inner fluxes

Example of a 3D hollow thermal tube with external temperatures and inner fluxes