Computational Methods and Experimental Measurements: by James T. P. Yao (auth.), G. A. Keramidas, C. A. Brebbia


By James T. P. Yao (auth.), G. A. Keramidas, C. A. Brebbia (eds.)

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Additional info for Computational Methods and Experimental Measurements: Proceedings of the International Conference, Washington D.C., July 1982

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Here statistical properties of the parameters of the computational model have to be taken into account which may be true in series production, or which are only a theoretical expedient. The estimations based on the Bayesian method etc. g. in /Eykhoff,P. K. D. et al. ( 1 9 72 ) I , but the information needed to apply these more sophisticated estimation methods is difficult to procure. 0 6 a a 0 a a Exact parameter value Estimated parameter value Values of the computational model Figure 1 Probability distributions of test and computational models with the exact parameter ~ 5.

G. (Editor) (1982) Identification of Vibrating Structures. CISM Lectur Notes, will appear in Springer-Verlag Wien. G. (1982) Einflihrung in Theorie und Praxis der Zeitreihen- und Modalanalyse: Identifikation schwingungsfahiger elastomechanischer Systeme,will appear in Vieweg-Verlag, Wiesbaden. G. (1977) Die Korrektur des Rechenmodells eines elastomechanischen Systems mittels gemessener erzwungener Schwingungen. Archiv 46: 169-184. G. (1981) Parameter Adjustment of a Model of an Offshore Platform from Estimated Eigenfre quencies Data.

01. 2: Resonance diagrams of the two models 31 When the damping D is light, the resonance peaks in v 3 occur approximately at the computed results (1). For an increasing damping, however, the peaks are appreciably shifted. Furthermore, they are decreasing in such a way that higher modes are no more measurable. Similar measurement difficulties we observe in the v 1 (~) of the two-degree-ofsmall values E, both peaks of freedom model. In case are not separated. Instead of the two natural fre- magnification functions quencies (2), only one resonance is measurable.

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