Consider the problem of a classical square vibrating membrane with all edges
fixed against transverse displacement. The differential equation of motion can
be written as:
where T is the initial tension in the membrane and
ρ
the area density. The boundary condition is that w vanishes on all the
edges of the membrane. Taking:

leads
to:

where l
=
rw2/T.
This is the Helmholtz problem on the square, with the dependent variable
y
prescribed as zero everywhere on the boundary. Model the top right-most
quadrant of the membrane using eight equally-sized 3-node triangles and compute
the associated eigenvalues and the eigenfunctions.

Note: Use a node numbering scheme that will make assembly of the stiffness
and mass matrices as simple as possible.
As a check on your work, if you assume a
= 1 and
rw2/T = 1,then
first two eigenvalues are 4.3889 and 33.6174.
The associated first two mode shapes are:


This web site was originally
developed by
Charles Camp for
CIVL
7111.
This site is
maintained by the
Department of Civil Engineering
at the University of Memphis.
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