What is the General Form of the Explicit Equations of Motion for Constrained Mechanical Systems?

Author:

Udwadia F. E.1,Kalaba R. E.2

Affiliation:

1. University of Southern California, Los Angeles, CA 90089-1453

2. University of Southern California, Los Angeles, CA 90089

Abstract

This paper presents the general form of the explicit equations of motion for mechanical systems. The systems may have holonomic and/or nonholonomic constraints, and the constraint forces may or may not satisfy D’Alembert’s principle at each instant of time. The explicit equations lead to new fundamental principles of analytical mechanics.

Publisher

ASME International

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference15 articles.

1. Lagrange, J. L., 1787, Mecanique Analytique, Mme Ve Courcier, Paris.

2. Gauss, C. F. , 1829, “Uber Ein Neues Allgemeines Grundgesetz der Mechanik,” J. Reine Agnew. Math., 4, pp. 232–235.

3. Gibbs, J. W. , 1879, “On the Fundamental Formulas of Dynamics,” Am. J. Math., 2, pp. 49–64.

4. Appell, P. , 1899, “Sur une forme generale des equations de la dynamique,” C. R. Acad. Sci., Paris, 129, pp. 459–460.

5. Poincare, H. , 1901, “Sur une forme nouvelle des equations de la mecanique,” C. R. Acad. Sci., Paris, 132, pp. 369–371.

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