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Volumn 19, Issue 1, 2009, Pages

The nonequilibrium ehrenfest gas: A chaotic model with flat obstacles?

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EID: 63849103149     PISSN: 10541500     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3085954     Document Type: Article
Times cited : (30)

References (27)
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    • As in Ref. 6, it is always difficult to decide whether these orbits are periodic or quasiperiodic.
    • As in Ref. 6, it is always difficult to decide whether these orbits are periodic or quasiperiodic.
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    • Incidentally, as common in nonequilibrium billiards (Ref. 5), the second Lyapunov exponent takes the same value as the first because the eigenvalues of the stability matrix are complex conjugate.
    • Incidentally, as common in nonequilibrium billiards (Ref. 5), the second Lyapunov exponent takes the same value as the first because the eigenvalues of the stability matrix are complex conjugate.
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    • The dissipation produced by the Gaussian thermostat sharply differentiates our dynamics from Hamiltonian dynamics, although both preserve the total energy. Indeed, in our case, the total energy equals the kinetic energy, which is a constant of motion.
    • The dissipation produced by the Gaussian thermostat sharply differentiates our dynamics from Hamiltonian dynamics, although both preserve the total energy. Indeed, in our case, the total energy equals the kinetic energy, which is a constant of motion.


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