2011
DOI: 10.1016/j.physa.2010.12.045
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Entropy production and thermal conductivity of a dilute gas

Abstract: It is known that the thermal conductivity of a dilute gas can be derived by using kinetic theory. We present here a new derivation by starting with two known entropy production principles: the steepest entropy ascent (SEA) principle and the maximum entropy production (MEP) principle. A remarkable feature of the new derivation is that it does not require the specification of the existence of the temperature gradient. The known result is reproduced in a similar form.

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Cited by 3 publications
(14 citation statements)
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“…where n is the number density. We thus recover the system entropy obtained in work [1]. Note that the system entropy here is about the dynamical randomness arising from molecular collisions.…”
Section: Specify Phenomenonsupporting
confidence: 56%
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“…where n is the number density. We thus recover the system entropy obtained in work [1]. Note that the system entropy here is about the dynamical randomness arising from molecular collisions.…”
Section: Specify Phenomenonsupporting
confidence: 56%
“…In the same way, we have |C down | 2 ∝ exp − aqE k B T . When the ion actually jumps, the superposition state collapses: the ion jumps either up with probability |C up | 2 or down with probability |C down | 2 , as shown in (1). The results of the two ways are different.…”
Section: Discussionmentioning
confidence: 99%
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“…which takes the same form as the entropy of a dilute gas that carries a heat flux [2] or a velocity gradient [3]. Using Eq.…”
Section: Entropy Methodsmentioning
confidence: 99%
“…(2) is obtained. We shall present in this letter a new derivation of the viscosity of a dilute gas, by analogy with a derivation of the thermal conductivity of a dilute gas [2]. The new derivation will use the entropy production.…”
Section: Introductionmentioning
confidence: 99%