Hamiltonians representing equations of motion with damping due to friction

Suppose that $H(q,p)$ is a Hamiltonian on a manifold M, and $\tilde L(q,\dot q)$, the Rayleigh dissipation function, satisfies the same hypotheses as a Lagrangian on the manifold M. We provide a Hamiltonian framework that gives the equation $$ \dot q = \frac{\partial H}{\partial p}(q,p) ,...

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Main Author: Stephen Montgomery-Smith
Format: Article
Language:English
Published: Texas State University 2014-04-01
Series:Electronic Journal of Differential Equations
Subjects:
Online Access:http://ejde.math.txstate.edu/Volumes/2014/89/abstr.html
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author Stephen Montgomery-Smith
author_facet Stephen Montgomery-Smith
author_sort Stephen Montgomery-Smith
collection DOAJ
description Suppose that $H(q,p)$ is a Hamiltonian on a manifold M, and $\tilde L(q,\dot q)$, the Rayleigh dissipation function, satisfies the same hypotheses as a Lagrangian on the manifold M. We provide a Hamiltonian framework that gives the equation $$ \dot q = \frac{\partial H}{\partial p}(q,p) , \quad \dot p = - \frac{\partial H}{\partial q}(q,p) - \frac{\partial \tilde L}{\partial \dot q}(q,\dot q) $$ The method is to embed M into a larger framework where the motion drives a wave equation on the negative half line, where the energy in the wave represents heat being carried away from the motion. We obtain a version of Nother's Theorem that is valid for dissipative systems. We also show that this framework fits the widely held view of how Hamiltonian dynamics can lead to the ``arrow of time.''
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spelling doaj.art-8b39324e3f7d42a297451dbe545537c22022-12-22T02:06:49ZengTexas State UniversityElectronic Journal of Differential Equations1072-66912014-04-01201489,110Hamiltonians representing equations of motion with damping due to frictionStephen Montgomery-Smith0 Univ. of Missouri, Columbia, MO, USA Suppose that $H(q,p)$ is a Hamiltonian on a manifold M, and $\tilde L(q,\dot q)$, the Rayleigh dissipation function, satisfies the same hypotheses as a Lagrangian on the manifold M. We provide a Hamiltonian framework that gives the equation $$ \dot q = \frac{\partial H}{\partial p}(q,p) , \quad \dot p = - \frac{\partial H}{\partial q}(q,p) - \frac{\partial \tilde L}{\partial \dot q}(q,\dot q) $$ The method is to embed M into a larger framework where the motion drives a wave equation on the negative half line, where the energy in the wave represents heat being carried away from the motion. We obtain a version of Nother's Theorem that is valid for dissipative systems. We also show that this framework fits the widely held view of how Hamiltonian dynamics can lead to the ``arrow of time.''http://ejde.math.txstate.edu/Volumes/2014/89/abstr.htmlHamiltonianLagrangianRayleigh dissipation functionfrictionNother's Theorem
spellingShingle Stephen Montgomery-Smith
Hamiltonians representing equations of motion with damping due to friction
Electronic Journal of Differential Equations
Hamiltonian
Lagrangian
Rayleigh dissipation function
friction
Nother's Theorem
title Hamiltonians representing equations of motion with damping due to friction
title_full Hamiltonians representing equations of motion with damping due to friction
title_fullStr Hamiltonians representing equations of motion with damping due to friction
title_full_unstemmed Hamiltonians representing equations of motion with damping due to friction
title_short Hamiltonians representing equations of motion with damping due to friction
title_sort hamiltonians representing equations of motion with damping due to friction
topic Hamiltonian
Lagrangian
Rayleigh dissipation function
friction
Nother's Theorem
url http://ejde.math.txstate.edu/Volumes/2014/89/abstr.html
work_keys_str_mv AT stephenmontgomerysmith hamiltoniansrepresentingequationsofmotionwithdampingduetofriction