An eigenfrequency study solves for the eigenfrequencies (natural frequencies) and the shapes of the corresponding eigenmodes.
Because only the shape and not the size of the modes (eigenvectors) have physical significance, the computed modes can be scaled arbitrarily. You can select the method for scaling in the Eigenvalue Solver node of the solver sequence. If output of
mass participation factors is required, then
Scaling of eigenvectors must be set to
Mass matrix. This means that the eigenmodes
U are orthogonalized with respect to the mass matrix
M so that
Here, dj is a vector containing unity displacement in all degrees of freedom representing translation in direction
j. The mass participation factor gives an indication of to which extent a certain mode might respond to an excitation in that direction.
The mass participation factors are available as a global variables, and these can be shown in a table using a Global Evaluation node under
Derived Values in the
Results branch, for example. The participation factor variables are available as predefined variables in the
Solver submenu.
It is possible to compute eigenfrequencies for structures which are not fully constrained; this is sometimes referred to as free-free modes. For each possible rigid body mode, there is one eigenvalue which in theory is zero. The number of possible rigid body modes for different geometrical dimensions is shown in the table below.
In a loaded structure, the natural frequencies may be shifted due to stress stiffening. With the
Prestressed Analysis, Eigenfrequency study type you can compute eigenfrequencies taking this effect into account.