A modified Lagrange method to analyze problems of sliding and rolling is presented. The method is based on modeling the friction as a process of collisions between the sliding and rolling body, and particles of the surface on which it slips and rolls. The process of collisions does not need to describe the exact friction process. Instead it can represent another equivalent mechanism of loss of energy of the body due to sliding and rolling. The function that describes the rate of increase of the kinetic energy of the particles, as a result of the collisions, plays a major roll in the modified Lagrange equations. Cases of isotropic and anisotropic friction can be modeled. Three examples of using the method are presented. It is shown that when an infinitely rough surface is assumed, the classical equations for nonholonomic constraints of rolling without sliding are obtained. Lagrange multipliers that appear in these equations obtain direct physical meaning and the mechanism behind the constraint becomes clear. [S0021-8936(00)01404-5]

1.
Neimark, I., Jr., and Fufaev, N. A., 1972, Dynamics of Nonholonomic Systems, The American Mathematical Society, Providence, RI (translation of the Russian book from 1967).
2.
Hamel, G., 1949, “Theoretische Mechanik,” Die Grundlehren der Mathematischen Wissenschaften in Ein Zeldarstellungen, Band LVII, Springer, Berlin, pp. 464–473.
3.
Oden
,
J. T.
, and
Martins
,
J. A. C.
,
1985
, “
Models and Computational Methods for Dynamic Friction Phenomena
,”
Comput. Methods Appl. Mech. Eng.
,
52
, pp.
527
634
.
4.
Banerjee
,
A. K.
, and
Kane
,
T. R.
,
1994
, “
Modeling and Simulation of Rotor Bearing Friction
,”
AIAA J. Guidance and Control
,
17
, No.
5
, pp.
1137
1139
.
5.
Bauchau
,
O. A.
,
1999
, “
On the Modeling of Friction and Rolling in Flexible Multi-Body Systems
,”
Multibody Syst. Dyn.
,
3
, pp.
209
239
.
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