In the dynamics of multibody systems that consist of interconnected rigid and deformable bodies, it is desirable to have a formulation that preserves the exactness of the rigid body inertia. As demonstrated in this paper, the incremental finite element approach, which is often used to solve large rotation problems, does not lead to the exact inertia of simple structures when they rotate as rigid bodies. Nonetheless, the exact inertia properties, such as the mass moments of inertia and the moments of mass, of the rigid bodies can be obtained using the finite element shape functions that describe large rigid body translations by introducing an intermediate element coordinate system. The results of application of the parallel axis theorem can be obtained using the finite element shape functions by simply changing the element nodal coordinates. As demonstrated in this investigation, the exact rigid body inertia properties in case of rigid body rotations can be obtained using the shape function if the nodal coordinates are defined using trigonometric functions. The analysis presented in this paper also demonstrates that a simple expression for the kinetic energy can be obtained for flexible bodies that undergo large displacements without the need for interpolation of large rotation coordinates.
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June 1996
Research Papers
Finite Element Incremental Approach and Exact Rigid Body Inertia
A. A. Shabana
A. A. Shabana
Department of Mechanical Engineering, University of Illinois at Chicago, 842 West Taylor Street, Chicago, IL 60607-7022
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A. A. Shabana
Department of Mechanical Engineering, University of Illinois at Chicago, 842 West Taylor Street, Chicago, IL 60607-7022
J. Mech. Des. Jun 1996, 118(2): 171-178 (8 pages)
Published Online: June 1, 1996
Article history
Received:
September 1, 1994
Revised:
December 1, 1995
Online:
December 11, 2007
Citation
Shabana, A. A. (June 1, 1996). "Finite Element Incremental Approach and Exact Rigid Body Inertia." ASME. J. Mech. Des. June 1996; 118(2): 171–178. https://doi.org/10.1115/1.2826866
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