2020
DOI: 10.48550/arxiv.2009.06883
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An autonomous out of equilibrium Maxwell's demon for controlling the energy fluxes produced by thermal fluctuations

Sergio Ciliberto
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Cited by 1 publication
(10 citation statements)
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“…which in turn imply T 4 < T 2 , i.e., the demon must have access to a reservoir with a temperature lower than the minimum temperature of the reservoirs in contact with the system. This is also the case in the examples in [18,19], and it can be seen that it is a general feature of linear [20]. Note that the condition J int = 0 implies J 2 = −J 1 , so a local observer that only has access to the values of J 1 and J 2 might jump to the conclusion these two are actually the same flow, which was reversed by the demon.…”
Section: An Elementary Examplementioning
confidence: 56%
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“…which in turn imply T 4 < T 2 , i.e., the demon must have access to a reservoir with a temperature lower than the minimum temperature of the reservoirs in contact with the system. This is also the case in the examples in [18,19], and it can be seen that it is a general feature of linear [20]. Note that the condition J int = 0 implies J 2 = −J 1 , so a local observer that only has access to the values of J 1 and J 2 might jump to the conclusion these two are actually the same flow, which was reversed by the demon.…”
Section: An Elementary Examplementioning
confidence: 56%
“…Given a partition separating the degrees of freedom of the system from those of the demon, we can also identify an internal energy current J int between them. In this context, the following conditions were proposed in [18,19] to characterize a 'nonequilibrium Maxwell demon': , in such a way that the currents J 1/2 are reversed. However, the current JS through the system remains invariant.…”
Section: General Settingmentioning
confidence: 99%
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