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Computational Science, Engineering & Technology Series
ISSN 1759-3158 CSETS: 12
PROGRESS IN ENGINEERING COMPUTATIONAL TECHNOLOGY Edited by: B.H.V. Topping, C.A. Mota Soares
Chapter 11
Analysis of Plastic Deformations in Multibody System Dynamics H. Sugiyama and A.A. Shabana
Department of Mechanical and Industrial Engineering, University of Illinois at Chicago, Illinois, United States of America H. Sugiyama, A.A. Shabana, "Analysis of Plastic Deformations in Multibody System Dynamics", in B.H.V. Topping, C.A. Mota Soares, (Editors), "Progress in Engineering Computational Technology", Saxe-Coburg Publications, Stirlingshire, UK, Chapter 11, pp 247-270, 2004. doi:10.4203/csets.12.11
Keywords: flexible multibody system dynamics, nonlinear finite element methods, large deformation, elasto-plasticity, joint constraints, computer simulations.
Summary
In the general theory of continuum mechanics, the state of rotation and
deformation of material points can be uniquely defined from the displacement field
by using the nine independent components of the displacement gradients. For this
reason, the use of the absolute rotation parameters as nodal coordinates, without
relating them to the displacement gradients, leads to coordinate redundancy that
leads to numerical and fundamental problems in many existing large rotation vector
formulations. No special measures need to be taken in order to satisfy the principle
of work and energy when the finite element absolute nodal coordinate formulation
is used. This formulation does not suffer from the problem of coordinate redundancy
and ensures the continuity of the stresses and strains at the nodal points. The
computer implementation of this formulation for multibody system applications is
discussed. A Lagrangian plasticity formulation that can be used with the absolute
nodal coordinate formulation in the analysis of flexible multibody dynamics is also
proposed. It is demonstrated that the principle of objectivity can be automatically
satisfied when the stress and strain rate are directly calculated using the Lagrangian
descriptions. This is attributed to the fact that, in the finite element absolute nodal
coordinate formulation, the position vector gradients can completely define the state
of rotation and deformation within the element.
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