Proper orthogonal decomposition (POD), also known as Karhunen}Loeve (K}L) decomposition, is emerging as a useful experimental tool in dynamics and vibrations. The POD is a means of extracting spatial information from a set of time-series data available on a domain. The use of (K}L) transform is of g
APPLICATION OF THE VARIABLE PROJECTION METHOD FOR UPDATING MODELS OF MECHANICAL SYSTEMS
โ Scribed by U. PRELLS; M.I. FRISWELL
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 231 KB
- Volume
- 225
- Category
- Article
- ISSN
- 0022-460X
No coin nor oath required. For personal study only.
โฆ Synopsis
To update the parameters of a mathematical model of a mechanical system usually a cost function is minimised which consists of the di!erence between calculated and measured quantities. This paper deals with the special case where the forces are unknown. Instead of following the usual way of handling this type of updating problem by assuming a model for the forces, in this paper the variable projection method is applied to estimate the unknown forces in addition to the model parameters. Under certain conditions this two-fold inverse problem can be solved by eliminating the force from the parameter estimation process. The remaining equation to estimate the model parameters consists of the projection of the response data, where the associated projector depends on the model parameters. This application of the variable projection method is essentially an extension of the output residual method and leads to an estimation equation which is non-linear with respect to the model parameters. The variable projection method is introduced and investigated for two general types of unknown forces. Two theoretical examples, wind excitation of a tower and a rotary machine under unknown unbalance con"guration, and the experimental case of a free}free steel beam tested by hammer excitation, are presented and discussed.
๐ SIMILAR VOLUMES
An application of the intermediate Hamiltonian method is reported in estimation of the lower bounds to the potential energy curve of the hydrogen molecule ion. An improvement of the method and its limitation are also discussed.