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Virtual nonlinear nonholonomic constraints from a symplectic point of view

Efstratios Stratoglou, Alexandre Anahory Simoes, Anthony Bloch, Leonardo Colombo

TL;DR

The paper develops a geometric characterization of virtual nonlinear nonholonomic constraints within a symplectic framework on $TQ$, showing that under a transversality condition there exists a unique feedback law that enforces the constraint manifold $\mathcal{M}$ and yields a closed-loop dynamics that satisfy a Chetaev-type equation. The main idea is to express dynamics via the symplectic form $\omega_L$ induced by a Lagrangian $L$ and the almost-tangent structure $J$, leading to a projection interpretation where the constrained motion is the projection of the uncontrolled dynamics onto $T\mathcal{M}$. A key result is that the closed-loop vector field obeys $i_{\Gamma}\omega_L - dE_L \in \flat_{\mathcal{G}^c}(\mathcal{F}^V)$, ensuring invariant virtual constraints, with explicit application to a controlled double pendulum showing energy dissipation and constraint behavior under simulation. This framework provides a rigorous geometric foundation for designing and analyzing virtual nonlinear nonholonomic constraints in Lagrangian control systems, linking variational structure to constraint satisfaction and controllable dynamics.

Abstract

In this paper, we provide a geometric characterization of virtual nonlinear nonholonomic constraints from a symplectic perspective. Under a transversality assumption, there is a unique control law making the trajectories of the associated closed-loop system satisfy the virtual nonlinear nonholonomic constraints. We characterize them in terms of the symplectic structure on $TQ$ induced by a Lagrangian function and the almost-tangent structure. In particular, we show that the closed-loop vector field satisfies a geometric equation of Chetaev type. Moreover, the closed-loop dynamics is obtained as the projection of the uncontrolled dynamics to the tangent bundle of the constraint submanifold defined by the virtual constraints.

Virtual nonlinear nonholonomic constraints from a symplectic point of view

TL;DR

The paper develops a geometric characterization of virtual nonlinear nonholonomic constraints within a symplectic framework on , showing that under a transversality condition there exists a unique feedback law that enforces the constraint manifold and yields a closed-loop dynamics that satisfy a Chetaev-type equation. The main idea is to express dynamics via the symplectic form induced by a Lagrangian and the almost-tangent structure , leading to a projection interpretation where the constrained motion is the projection of the uncontrolled dynamics onto . A key result is that the closed-loop vector field obeys , ensuring invariant virtual constraints, with explicit application to a controlled double pendulum showing energy dissipation and constraint behavior under simulation. This framework provides a rigorous geometric foundation for designing and analyzing virtual nonlinear nonholonomic constraints in Lagrangian control systems, linking variational structure to constraint satisfaction and controllable dynamics.

Abstract

In this paper, we provide a geometric characterization of virtual nonlinear nonholonomic constraints from a symplectic perspective. Under a transversality assumption, there is a unique control law making the trajectories of the associated closed-loop system satisfy the virtual nonlinear nonholonomic constraints. We characterize them in terms of the symplectic structure on induced by a Lagrangian function and the almost-tangent structure. In particular, we show that the closed-loop vector field satisfies a geometric equation of Chetaev type. Moreover, the closed-loop dynamics is obtained as the projection of the uncontrolled dynamics to the tangent bundle of the constraint submanifold defined by the virtual constraints.

Paper Structure

This paper contains 5 sections, 7 theorems, 13 equations, 1 figure.

Key Result

lemma thmcounterlemma

For a Riemannian metric $\mathcal{G}$ on $Q$, vector fields $X,Y\in\mathfrak{X}(Q)$ and a one-form $\alpha\in\Omega^1(Q)$ we have

Figures (1)

  • Figure :

Theorems & Definitions (20)

  • definition thmcounterdefinition
  • lemma thmcounterlemma
  • proof
  • proposition thmcounterproposition
  • proof
  • remark thmcounterremark
  • definition thmcounterdefinition
  • definition thmcounterdefinition
  • theorem thmcountertheorem
  • lemma thmcounterlemma
  • ...and 10 more