Abstract
The dynamic stiffness method enables one to model an infinite number of natural modes by means of a finite number of degrees of freedom. The method has been extended to frame structures with uniform or non-uniform, straight or curved, damped or undamped beam members. An orthonormal condition is suggested here for the natural modes resulting from the dynamic stiffness method; modal analysis in the classical sense is then made possible. Modes corresponding to repeated natural frequencies are discussed in detail. An expansion theorem for expanding from a finite number of degrees of freedom by means of an infinite number of modes is validated by means of the frequency-dependent shape functions. Distributed modal participation factors are introduced for distributed excitations.
| Original language | English |
|---|---|
| Pages (from-to) | 125-137 |
| Journal | Dynamics and Stability of Systems |
| Volume | 2 |
| Issue number | 2 |
| DOIs | |
| Publication status | Published - Jan 1987 |
| Externally published | Yes |
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