Showing posts with label Modal Analysis. Show all posts
Showing posts with label Modal Analysis. Show all posts

Sunday, 15 April 2012

FEA Solver background of Modal analysis


The equilibrium equation for a structure performing free vibration appears as the eigenvalue problem:

     [K-λM]x = 0
where K is the stiffness matrix of the structure and M is the mass matrix.  Damping is neglected.  The solution of the eigenvalue problem yields n eigenvalues λ, where n is the number of degrees of freedom.  The vector x is the eigenvector corresponding to the eigenvalue.
The eigenvalue problem is solved using a matrix method called the Lanczos method.  Not all eigenvalues are required -- only a small number of the lowest eigenvalues are normally calculated.

The natural frequency fi follows directly from the eigenvalue λ.

 
In NASTRAN solver, in order to run a normal modes analysis, an EIGRL bulk data entry needs to be given because it defines the number of modes to be extracted.  The EIGRL card needs to be referenced by a METHOD statement in a SUBCASE in the subcase information section.