Abstract
The aim of this work is to show the possibility of using any dynamical codes devoted to rigid multibody systems in which the motion equations are obtained from the d'Alembert Principle, for the simulation of flexible multibody systems in which the flexible components are discretized by a Rayleigh–Ritz procedure. The results obtained are a generalization of the work done by Botz and Hagedorn [1] for planar elastic mechanisms. An application of the method is done using the symbolic dynamical code AUTOLEV [2].
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