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For the most basic problem involving a linear elastic material which obeys [[Hooke's Law]],
the [[Matrix (mathematics)|matrix]] equations take the form of a dynamic three dimensional spring mass system.
The generalized equation of motion is given as:<ref>
McGraw-Hill Publishing Company, New York, 1993, page 173
:<math>
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This is the general form of the eigensystem encountered in structural
engineering using the [[FEM]]. To represent the free-vibration solutions of the structure harmonic motion is assumed
is taken to equal <math>\lambda [U]</math>,
where <math>\lambda</math> is an eigenvalue (with units of reciprocal time squared, e.g., <math>\mathrm{s}^{-2}</math>),
and the equation reduces to:<ref>
McGraw-Hill Publishing Company, New York, 1993, page 201
:<math>[M][U] \lambda + [K][U] = [0]</math>
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multiplied through by the inverse of the mass,
<math> [M]^{-1} </math>,
it will take the form of the latter.<ref>
Applications'', 3rd Ed., Prentice-Hall Inc., Englewood Cliffs, 1988, page 165
Because the lower modes are desired, solving the system
more likely involves the equivalent of multiplying through by the inverse of the stiffness,
<math> [K]^{-1} </math>, a process called [[inverse iteration]].<ref>
Englewood Cliffs, 1987 page 582-584
When this is done, the resulting eigenvalues, <math> \mu </math>, relate to that of the original by:
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== Footnotes ==
{{Reflist}}
== References ==
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==External links==
*[http://frame3dd.sourceforge.net/ Frame3DD open source 3D structural modal analysis program]
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