Civil Engineering Reference
In-Depth Information
Three-dimensional problems are solved in Chapter 12, in which the displacements in
the z -direction are given by w .
2.19 Conclusions
When viewed from a finite element standpoint, all static equilibrium problems, whether
involving solids or fluids, take the same form, namely,
[ k m ]
{
u
} = {
f
}
(2.142)
or
{ φ } = {
}
[ k c ]
q
(2.143)
For simple uncoupled problems the solid [ k m ] and fluid [ k c ] matrices have similar
symmetrical structures, so computer programs to construct them will also be similar. How-
ever, for other problems, for example those described by the Navier-Stokes equations,
the constitutive matrices are unsymmetrical and appropriate alternative software will be
necessary.
In the same way, eigenvalue, propagation and transient problems all involve the mass
matrix [ m m ] (or a simple multiple of it). Therefore, coding of these different types of
solutions can be expected to contain sections common to all three problems.
So far, single elements have been considered in the discretisation process, and only
the simplest line and rectangular elements have been described. The next chapter is mainly
devoted to a description of programming strategy, but before this, the finite element concept
is extended to embrace meshes of interlinked elements and elements of general shape.
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