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Discrete Dirac structures and discrete Lagrange--Dirac dynamical systems in mechanics

Linyu Peng, Hiroaki Yoshimura

TL;DR

This paper develops a comprehensive discrete Dirac framework by introducing $(\pm)$-discrete Dirac structures on manifolds and their induced structures on $T^*Q$, enabling a discrete Lagrange--Dirac formalism. It defines discrete two-forms, discrete constraint spaces, and $(\pm)$-finite difference maps, then constructs Tulczyjew-like discrete triples and Dirac differentials to derive $(\pm)$-discrete Lagrange--Dirac equations via $(\pm)$-discrete Lagrange--d'Alembert--Pontryagin principles. The authors show equivalence of the resulting equations with established discrete Lagrange--d'Alembert equations, ensure preservation of the $(\pm)$-discrete induced Dirac structures in nonholonomic integrators, and validate the approach with numerical tests on a vertical rolling disk and a classical Heisenberg system. The work provides a robust, structure-preserving discretization strategy for nonholonomic mechanics and lays groundwork for extensions to discrete Hamilton–Dirac systems and higher-dimensional/thermodynamic settings. Overall, it offers a unified geometric and variational pathway to accurately simulate constrained mechanical systems in a discrete setting.

Abstract

In this paper, we propose the concept of $(\pm)$-discrete Dirac structures over a manifold, where we define $(\pm)$-discrete two-forms on the manifold and incorporate discrete constraints using $(\pm)$-finite difference maps. Specifically, we develop $(\pm)$-discrete induced Dirac structures as discrete analogues of the induced Dirac structure on the cotangent bundle over a configuration manifold, as described by Yoshimura and Marsden (2006). We demonstrate that $(\pm)$-discrete Lagrange--Dirac systems can be naturally formulated in conjunction with the $(\pm)$-induced Dirac structure on the cotangent bundle. Furthermore, we show that the resulting equations of motion are equivalent to the $(\pm)$-discrete Lagrange--d'Alembert equations proposed in Cortés and Martínez (2001) and McLachlan and Perlmutter (2006). We also clarify the variational structures of the discrete Lagrange--Dirac dynamical systems within the framework of the $(\pm)$-discrete Lagrange--d'Alembert--Pontryagin principle. Finally, we validate the proposed discrete Lagrange--Dirac systems with some illustrative examples of nonholonomic systems through numerical tests.

Discrete Dirac structures and discrete Lagrange--Dirac dynamical systems in mechanics

TL;DR

This paper develops a comprehensive discrete Dirac framework by introducing -discrete Dirac structures on manifolds and their induced structures on , enabling a discrete Lagrange--Dirac formalism. It defines discrete two-forms, discrete constraint spaces, and -finite difference maps, then constructs Tulczyjew-like discrete triples and Dirac differentials to derive -discrete Lagrange--Dirac equations via -discrete Lagrange--d'Alembert--Pontryagin principles. The authors show equivalence of the resulting equations with established discrete Lagrange--d'Alembert equations, ensure preservation of the -discrete induced Dirac structures in nonholonomic integrators, and validate the approach with numerical tests on a vertical rolling disk and a classical Heisenberg system. The work provides a robust, structure-preserving discretization strategy for nonholonomic mechanics and lays groundwork for extensions to discrete Hamilton–Dirac systems and higher-dimensional/thermodynamic settings. Overall, it offers a unified geometric and variational pathway to accurately simulate constrained mechanical systems in a discrete setting.

Abstract

In this paper, we propose the concept of -discrete Dirac structures over a manifold, where we define -discrete two-forms on the manifold and incorporate discrete constraints using -finite difference maps. Specifically, we develop -discrete induced Dirac structures as discrete analogues of the induced Dirac structure on the cotangent bundle over a configuration manifold, as described by Yoshimura and Marsden (2006). We demonstrate that -discrete Lagrange--Dirac systems can be naturally formulated in conjunction with the -induced Dirac structure on the cotangent bundle. Furthermore, we show that the resulting equations of motion are equivalent to the -discrete Lagrange--d'Alembert equations proposed in Cortés and Martínez (2001) and McLachlan and Perlmutter (2006). We also clarify the variational structures of the discrete Lagrange--Dirac dynamical systems within the framework of the -discrete Lagrange--d'Alembert--Pontryagin principle. Finally, we validate the proposed discrete Lagrange--Dirac systems with some illustrative examples of nonholonomic systems through numerical tests.

Paper Structure

This paper contains 93 sections, 5 theorems, 247 equations, 20 figures.

Key Result

Theorem 5.7

Let $\Omega_{M}^{d\pm}$ be the discrete two-form given in Def. DiscTwoForm_M and let $\Delta_{M}^{d\pm}$ be the discrete constraint spaces given in Def. DiscConstraintSpace_M. Then, the $(+)$-discrete structure $D^{d+}_{M} \subset (M\times M)\times T^{\ast}M$ that is defined by, for each $x_{1} \in is a Dirac structure on $M$. Further, the $(-)$-discrete structure $D^{d-}_{M} \subset (M\times M)\

Figures (20)

  • Figure 1: Variations $\delta q(t)$ of a curve $q(t)$.
  • Figure 2: Discrete sequences.
  • Figure 3: The bundle picture of the iterated tangent and cotangent bundles.
  • Figure 4: $(+)$-discrete bundle picture.
  • Figure 5: $(-)$-discrete bundle picture.
  • ...and 15 more figures

Theorems & Definitions (40)

  • Definition 3.1
  • Remark 4.1
  • Definition 4.2
  • Definition 5.1
  • Remark 5.2
  • Definition 5.3
  • Definition 5.4
  • Definition 5.5
  • Definition 5.6
  • Theorem 5.7
  • ...and 30 more