Intrinsic Time Integration Procedures for Rigid Body Dynamics

The treatment of rotations in rigid body and Cosserat solidsdynamics is challenging. In most cases, at some point in the formulation, a parameterization of rotation isintroduced and the intrinsic nature of the equations of motions is lost. Typically, this step considerably complic ates the form of the equations and increases the order of the nonlinearities. Clearly, it is desirable to bypass para meterization of rotation, leaving the equations of motion in their original, intrinsic form. This has prompted the dev elopment of rotationless and intrinsic formulations. This paper focuses on the latter approach. The most famous exampl e of intrinsic formulation is probably Euler’s second law for the motion of a rigid body rotating about an inertial p This equation involves angular velocities solely, with algebraic nonlinearities of the second-order at most.Unfortunately, this intrinsic equation also suffers serio us drawbacks: the angular velocity of the body is computed, butnot its orientation, the body is “unaware” of its inertial orientation. This paper presents an alternative a pproach to the problem by proposing discrete statements of the rotation kinematic compatibility equation, which prov ide solutions for both rotation tensor and angular velocity without relying on a parameterization of rotation. The form ulation is also generalized using the motion formalism, leading to very simple discretized equations of motion.