1981
DOI: 10.1002/zamm.19810611202
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Coulomb Friction in Two‐Dimensional Rigid Body Systems

Abstract: Die Lösungen des Coulombschen Reibungsproblems für starre Körper in zwei Dimensionen werden analysiert. Das bestimmende System von gewöhnlichen Differentialgleichungen und Ungleichungen wird aufgestellt. Beispiele werden vorgelegt, die einige ungewünschte Eigenschaften dieses speziellen Reibungsgesetzes nachweisen. Hinreichende Bedingungen für Existenz und Eindeutigkeit werden mit Hilfe der Theorie der linearen Komplementarität hergeleitet.

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Cited by 223 publications
(131 citation statements)
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“…This paper represents a step toward the development of improved engineering design tools for mechanical systems with unilateral contact. Following in the footsteps of Lötstedt and others who have popularized the use of complementarity methods in rigid body dynamics [7,8,11], we extend the model developed formally in [15] to include a frictional moment (transmitted about the contact normal). While it is not possible to transmit such a moment through a point contact (as would occur generically between curved rigid bodies), we include it in our model in recognition of the fact that contacts between stiff real bodies are distributed over small patches [6] and that the friction forces obey the maximum work inequality [5].…”
Section: Introductionmentioning
confidence: 99%
“…This paper represents a step toward the development of improved engineering design tools for mechanical systems with unilateral contact. Following in the footsteps of Lötstedt and others who have popularized the use of complementarity methods in rigid body dynamics [7,8,11], we extend the model developed formally in [15] to include a frictional moment (transmitted about the contact normal). While it is not possible to transmit such a moment through a point contact (as would occur generically between curved rigid bodies), we include it in our model in recognition of the fact that contacts between stiff real bodies are distributed over small patches [6] and that the friction forces obey the maximum work inequality [5].…”
Section: Introductionmentioning
confidence: 99%
“…In the next simulation step the contact surface of the initial simulation is re-shaped according to the wear-rate function r W (16). The maximum used change of body shape is u Max = 0.15 μm.…”
Section: Run-in Period (Wear)mentioning
confidence: 99%
“…The first studies of unilateral contacts in the form of a linear complementarity problem were published by Lötstedt [16,17].…”
Section: Introductionmentioning
confidence: 99%
“…Timestepping methods, which have their origins in early 80's [17], were developed to overcome some of these difficulties. The contact state (rolling, sliding or no contact) at each contact is allowed to change at any time, and the transitions between contact states are described by complementarity constraints on the relative positions (or their derivatives) and contact forces (or their integrals).…”
Section: Introductionmentioning
confidence: 99%