2017
DOI: 10.1088/1361-6544/aa85d6
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Energy dissipation in Hamiltonian chains of rotators

Abstract: We discuss, in the context of energy flow in high-dimensional systems and Kolmogorov-Arnol'd-Moser (KAM) theory, the behavior of a chain of rotators (rotors) which is purely Hamiltonian, apart from dissipation at just one end. We derive bounds on the dissipation rate which become arbitrarily small in certain physical regimes, and we present numerical evidence that these bounds are sharp. We relate this to the decoupling of non-resonant terms as is known in KAM problems.

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Cited by 16 publications
(32 citation statements)
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“…We now recall in more detail the situation considered in [4]. The authors start from a Hamiltonian system of N rotators coupled to their nearest neighbors.…”
Section: Jean-pierre Eckmann and C Eugene Waynementioning
confidence: 99%
See 2 more Smart Citations
“…We now recall in more detail the situation considered in [4]. The authors start from a Hamiltonian system of N rotators coupled to their nearest neighbors.…”
Section: Jean-pierre Eckmann and C Eugene Waynementioning
confidence: 99%
“…We will focus primarily on the case N = 3 for simplicity, but in principle, our methods apply to systems with arbitrarily many degrees of freedom, and we plan to return to the consideration of the general case in a future work. We will choose initial conditions for this system in which essentially all of the energy is in mode u 1 , and will add a weak dissipative term to the last mode as in [4] by adding to Eq. (1) a term of the form…”
Section: Jean-pierre Eckmann and C Eugene Waynementioning
confidence: 99%
See 1 more Smart Citation
“…1 For chains of length n, it is conjectured in [3, Remark 5.3] that the exponent is 1/(2 n/2 − 2), which is indeed 1/2 when n = 3, 4. This conjecture is supported by [5], where the rate of energy dissipation in deterministic chains of rotors of arbitrary lengths is studied.…”
mentioning
confidence: 85%
“…We will choose initial conditions for this system in which essentially all of the energy is in mode u 1 , and will add a weak dissipative term to the last mode as in [1,2] by adding to Eq. (1.1) a term of the form iγ δ n, j u j ,…”
Section: Introductionmentioning
confidence: 99%