Rough collision in three-dimensional rigid multi-body systems

Abstract In the current paper, single point rough collision in three-dimensional rigid multibody systems is modelled. Coulomb's friction law and infinite tangential stiffness are assumed. Routh's incremental model with energetic coefficient of restitution is used. Equations of motion are developed by means of Lagrangian formulation. The non-linear equations of motion show that the contact point could continuously change its sliding direction or the sliding could halt and the non-sliding persists or it could restart along a new direction. All these possible sliding behaviours during impact are identified, conditions leading to each behaviour are specified, and an appropriate numerical procedure is suggested. Normal impulse at the contact point is considered the independent variable, as time-like, to carry out the numerical integrations of the equations of motion. A case of a four-degrees-of-freedom spatial robot that collides with its environment is investigated. Solutions describing the variation of collision variables are obtained. It is recognized that qualitative changes to all the variables occur whenever sliding velocity reaches its minimum value. These critical spots are identified, the associated abrupt variations in the impact variables are explored and the friction influence is observed.

[1]  R. I. Leine,et al.  Nonlinear Dynamics and Modeling of Various Wooden Toys with Impact and Friction , 2003 .

[2]  Jeff Koechling,et al.  Partitioning the Parameter Space According to Different Behaviors During Three-Dimensional Impacts , 1995 .

[3]  V. Bhatt,et al.  Three-Dimensional Frictional Rigid-Body Impact , 1995 .

[4]  Jeffrey C. Trinkle,et al.  Complementarity formulations and existence of solutions of dynamic multi-rigid-body contact problems with coulomb friction , 1996, Math. Program..

[5]  Mark Moll,et al.  Manipulation of Pose Distributions , 2002, Int. J. Robotics Res..

[6]  Dinesh K. Pai,et al.  Fast frictional dynamics for rigid bodies , 2005, SIGGRAPH 2005.

[7]  W. Stronge Rigid body collisions with friction , 1990, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[8]  E. Pennestrì,et al.  Multibody dynamics simulation of planar linkages with Dahl friction , 2007 .

[9]  David Baraff,et al.  Coping with friction for non-penetrating rigid body simulation , 1991, SIGGRAPH.

[10]  M. T. Mason,et al.  Two-Dimensional Rigid-Body Collisions With Friction , 1992 .

[11]  W. Stronge Swerve During Three-Dimensional Impact of Rough Rigid Bodies , 1994 .

[12]  A. Ruina,et al.  A New Algebraic Rigid-Body Collision Law Based on Impulse Space Considerations , 1998 .

[13]  Edmund Taylor Whittaker,et al.  A Treatise on the Analytical Dynamics of Particles and Rigid Bodies: INDEX OF TERMS EMPLOYED , 1988 .

[14]  Mark W. Spong,et al.  Control of Planar Rigid Body Sliding with Impacts and Friction , 2000, Int. J. Robotics Res..

[15]  Jorge Ambrósio,et al.  Influence of the contact—impact force model on the dynamic response of multi-body systems , 2006 .

[16]  Joaquim A. Batlle,et al.  On Newtons and Poissons Rules of Percussive Dynamics , 1993 .

[17]  Victor J. Milenkovic,et al.  A fast impulsive contact suite for rigid body simulation , 2004, IEEE Transactions on Visualization and Computer Graphics.

[18]  Termination conditions for three-dimensional inelastic collisions in multibody systems , 2001 .

[19]  Werner Schiehlen,et al.  Three Approaches for Elastodynamic Contact in Multibody Systems , 2004 .

[20]  J. A. Batlle The sliding velocity flow of rough collisions in multibody systems , 1996 .