2022
DOI: 10.1063/5.0073214
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Geometric Hamilton–Jacobi theory for systems with external forces

Abstract: In this paper, we develop a Hamilton–Jacobi theory for forced Hamiltonian and Lagrangian systems. We study the complete solutions, particularize for Rayleigh systems, and present some examples. Additionally, we present a method for the reduction and reconstruction of the Hamilton–Jacobi problem for forced Hamiltonian systems with symmetry. Furthermore, we consider the reduction of the Hamilton–Jacobi problem for a Čaplygin system to the Hamilton–Jacobi problem for a forced Lagrangian system.

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Cited by 5 publications
(4 citation statements)
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References 58 publications
(54 reference statements)
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“…This is the discrete analogue of the first statement from our reduction lemma [6, lemma 15] (see also references [7,21]). The first statement was previously found by Marsden and West [23, theorem 3.2.1].…”
Section: If This Equation Holds F D Is ξ-Invariant If and Only Ifmentioning
confidence: 63%
See 1 more Smart Citation
“…This is the discrete analogue of the first statement from our reduction lemma [6, lemma 15] (see also references [7,21]). The first statement was previously found by Marsden and West [23, theorem 3.2.1].…”
Section: If This Equation Holds F D Is ξ-Invariant If and Only Ifmentioning
confidence: 63%
“…Remark 1. It is worth noting that we have changed the sign criteria for discrete forces with respect to our previous papers [6,7,21], in order to be consistent with Lew, Marsden, Ortiz and West's criteria [20,23].…”
Section: Lagrangian Systems With External Forcesmentioning
confidence: 99%
“…There is a nice way to employ external forces to Hamiltonian dynamics. For the dynamical systems admitting some external forces, geometric HJ theory is studied in [5,50,99].…”
Section: An Incomplete Literature On Geometric Hamilton-jacobi Theorymentioning
confidence: 99%
“…on the cotangent bundle, called Darboux coordinates, on cotangent bundle T * Q such that the canonical one form turns out to be Θ Q = p i dq i , whereas the canonical symplectic two-form in (50) becomes…”
Section: Space Of Hamiltonian Vector Fields (Revisited)mentioning
confidence: 99%