Screw and Lie Group Theory in Multibody Dynamics -- Recursive Algorithms and Equations of Motion of Tree-Topology Systems

TL;DR

This paper introduces recursive algorithms and equations of motion for multibody systems using screw and Lie group theory, emphasizing computational efficiency, frame invariance, and higher-order derivatives for dynamic analysis.

Contribution

It develops recursive $O(n)$ Newton-Euler algorithms for various twist representations and derives closed-form motion equations using Lie group formulations, enhancing multibody dynamics modeling.

Findings

Recursive algorithms for twists, accelerations, and wrenches are derived.

Closed-form multibody motion equations are formulated using Lie groups.

Extensions to higher-order derivatives enable advanced dynamic analysis.

Abstract

Screw and Lie group theory allows for user-friendly modeling of multibody systems (MBS) while at the same they give rise to computationally efficient recursive algorithms. The inherent frame invariance of such formulations allows for use of arbitrary reference frames within the kinematics modeling (rather than obeying modeling conventions such as the Denavit-Hartenberg convention) and to avoid introduction of joint frames. The computational efficiency is owed to a representation of twists, accelerations, and wrenches that minimizes the computational effort. This can be directly carried over to dynamics formulations. In this paper recursive $O\left( n\right) $ Newton-Euler algorithms are derived for the four most frequently used representations of twists, and their specific features are discussed. These formulations are related to the corresponding algorithms that were presented in the literature. The MBS motion equations are derived in closed form using the Lie group formulation. One are the so-called 'Euler-Jourdain' or 'projection' equations, of which Kane's equations are a special case, and the other are the Lagrange equations. The recursive kinematics formulations are readily extended to higher orders in order to compute derivatives of the motions equations. To this end, recursive formulations for the acceleration and jerk are derived. It is briefly discussed how this can be employed for derivation of the linearized motion equations and their time derivatives. The geometric modeling allows for direct application of Lie group integration methods, which is briefly discussed.