The equations of motion of a multibody system are linearized and reduced to independent coordinates, using an orthogonal complement method. The orthogonal complement is used to eliminate the terms that result from a variation of the constraint forces. The resulting equations contain the derivative of the constraint Jacobian with respect to the coordinate vector in the stiffness matrix. The technique is suitable for a computer implementation. Examples are used to illustrate the process.
Amirouche, F. M. L. , 1992, Computational Methods in Multibody Dynamics, Prentice-Hall, Englewood Cliffs, NJ .
2.
Greenwood, D. T. , 1988, Principles of Dynamics, Prentice-Hall, Englewood Cliffs, NJ .
3.
Lieh, J. and Haque, I. , 1991, “Symbolic closed-form modeling and linearization of multibody systems subject to control,”Journal of Mechanical Design113, 124-132 .
4.
Lynch, A. G. and Vanderploeg, M. J. , 1995, “A symbolic formulation for linearization of multibody equations of motion,”Journal of Mechanical Design117, 441-445 .
5.
Nikravesh, P. E. , 1988, Computer-Aided Analysis of Mechanical Systems, Prentice-Hall, Englewood Cliffs, NJ .
6.
Nikravesh, P. E. and Gim, G. , 1993, “Systematic construction of the equations of motion for multibody systems containing closed kinematic loops,”Journal of Mechanical Design115, 143-149 .
7.
Ogata, K. , 1990, Modern Control Engineering, Prentice-Hall, Englewood Cliffs, NJ .
8.
Saha, S. K. and Angeles, J. , 1991, “Dynamics of non-holonomic mechanical systems using a natural orthogonal complement,”Journal of Applied Mechanics58, 238-243 .
9.
Shabana, A. A. , 1994, Computational Dynamics, Wiley, NY .
10.
Wampler, C. , Buffinton, K. , and Shu-hui, J. , 1985, “Formulation of equations of motion for systems subject to constraints,”Journal of Applied Mechanics52, 465-470 .
11.
Wehage, R. A. and Haug, E. J. , 1982, “Generalized coordinate partitioning for dimension reduction in analysis of constrained dynamic systems,”Journal of Mechanical Design104, 247-255 .