The differential equations for planar impacts reduce to an algebraic form,and can be easily solved.For three dimensional impacts with friction,there is no closed-form solution,and numerical integration is required due...The differential equations for planar impacts reduce to an algebraic form,and can be easily solved.For three dimensional impacts with friction,there is no closed-form solution,and numerical integration is required due to the swerve behavior of tangential impulse during collisions.The dynamic governing equations in the impact process are built up in impulse space based on the Lagrangian equation in this paper.The coefficient of restitution defined by Poisson is used as the condition of impact termination.A valid nu-merical method for solving three-dimensional frictional impact of multi-rigid body system is established.The singular cases of tangential movement in sticking point are especially noticed and analyzed.Several examples are present to reveal the different kinds of tan-gential movement modes varied with the normal impulse during collision.展开更多
基金the National Natural Science Foundation of China(Grant Nos.10272002,10502009,60334030)the Natural Science Foundation of Beijing(Grant No.1062007).
文摘The differential equations for planar impacts reduce to an algebraic form,and can be easily solved.For three dimensional impacts with friction,there is no closed-form solution,and numerical integration is required due to the swerve behavior of tangential impulse during collisions.The dynamic governing equations in the impact process are built up in impulse space based on the Lagrangian equation in this paper.The coefficient of restitution defined by Poisson is used as the condition of impact termination.A valid nu-merical method for solving three-dimensional frictional impact of multi-rigid body system is established.The singular cases of tangential movement in sticking point are especially noticed and analyzed.Several examples are present to reveal the different kinds of tan-gential movement modes varied with the normal impulse during collision.
