Mode Superposition
Analyzing forced dynamic response for large models can be very time-consuming. You can often improve the performance dramatically by using the mode superposition technique. The following requirements must be met for a modal solution to be possible:
When using the Structural Mechanics Module, there are four predefined study types for mode superposition:
The two first of these study types consist of two study steps: One step for computing the eigenfrequencies and one step for the modal response. The two latter have three study steps. Before the eigenfrequency step, you solve a static load case in order to get a prestress state used in the eigenfrequency computation.
In practice, you have often computed the eigenfrequencies already, and then want to use them in a mode superposition. In this case, start by adding an empty study, and then add a Time Dependent, Modal or Frequency Domain, Modal study step to it. After having added the study step this way, you must point the modal solver to the solution containing the eigenfrequencies and eigenmodes. You do this by first selecting Show default solver at the study level, and then selecting the eigenfrequency solution to be used in the Eigenpairs section of the generated modal solver.
In a mode superposition, the deformation of the structure is represented by a linear combination of its eigenmodes. The amplitudes of these modes are the degrees of freedom of the reduced problem. You must select which eigenmodes to include in the analysis. This choice is usually based on a comparison between the eigenfrequencies of the structure and the frequency content of the load. As a rule of thumb, select eigenmodes up to approximately twice the highest frequency of the excitation.
In the mode superposition formulation in COMSOL, the full model is projected onto the subspace spanned by the eigenmodes. A problem having the number of degrees equal to the number of included modes is then solved. Note that this differs from many implementations of mode superposition, where it often is assumed that the modal equations are totally decoupled.
An implication of this, is that it is not necessary to assume a certain structure of the damping matrix. Any type of damping which is allowable in the corresponding analysis of the full system can also be used in the modal based analysis.
For many common cases, the mode superposition analysis is not sensitive to whether the eigenmodes were computed using damping or not. The reason is that the eigenmodes of problems with Rayleigh damping and loss factor damping can be shown to be identical to those of the undamped problem, so that the projection to the subspace spanned by the eigenmodes is the same in both cases. For more general damping, it is however recommended that you suppress all contributions to the damping during the eigenfrequency step, and thus base the mode superposition on the solution to the undamped eigenfrequency problem.
Frequency Domain Analysis
All loads are assumed to have a harmonic variation. This is a perturbation type analysis, so only loads having the Harmonic perturbation property selected are then included in the analysis.
Time-Dependent Analysis
Only the factor of the load which is independent of time should be specified in the load features. The dependency on time is specified as Load factor under the Advanced section of the modal solver. This factor is then applied to all loads.
Modal Solver and Studies and Solvers in the COMSOL Multiphysics Reference Manual
For an example showing how to perform mode superposition in time and frequency domain, see Various Analyses of an Elbow Bracket: Application Library path Structural_Mechanics_Module/Tutorials/elbow_bracket.