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.)
Read Online or Download Computational Methods and Experimental Measurements: Proceedings of the International Conference, Washington D.C., July 1982 PDF
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Additional info for Computational Methods and Experimental Measurements: Proceedings of the International Conference, Washington D.C., July 1982
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.