2013
DOI: 10.3390/e15104243
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Conditioning, Correlation and Entropy Generation in Maxwell’s Demon

Abstract: Maxwell's Demon conspires to use information about the state of a confined molecule in a Szilard engine (randomly frozen into a state subspace by his own actions) to derive work from a single-temperature heat bath. It is widely accepted that, if the Demon can achieve this at all, he can do so without violating the Second Law only because of a counterbalancing price that must be paid to erase information when the Demon's memory is reset at the end of his operating cycle. In this paper, Maxwell's Demon is analyz… Show more

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Cited by 3 publications
(4 citation statements)
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“…There exists a vast amount of literature on Maxwell's demon and related questions [10,11,20]. Among them is an article that comes rather close to the results of the present work, namely [21], that deals with Szilard's engine and where we read in the abstract:…”
Section: Connections To the Olr Approachmentioning
confidence: 52%
“…There exists a vast amount of literature on Maxwell's demon and related questions [10,11,20]. Among them is an article that comes rather close to the results of the present work, namely [21], that deals with Szilard's engine and where we read in the abstract:…”
Section: Connections To the Olr Approachmentioning
confidence: 52%
“…There exists a vast amount of literature on Maxwell's demon and related questions [19]. Among them is an article that comes rather close to the results of the present work, namely [15], that deals with Szilard's engine and where we read in the abstract:…”
Section: Connections To the Olr Approachmentioning
confidence: 54%
“…Following [4] we want to explicitly construct a measurement dilation of J of the form (15), see also the analogous construction for a Maxwell instrument in [1].…”
Section: Lemmamentioning
confidence: 99%
“…This implies that all intensive variables in the surroundings are spatially uniform, an idealization which is at the core of the definition of reservoir in thermodynamics, the distinction between a work reservoir and heat reservoir being related with its entropy. A work reservoir does not change its entropy as it interacts with the system [6,7], unlike a heat reservoir which interacts with the system by experiencing an entropy variation S e D given by [5,6]…”
mentioning
confidence: 99%