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Equation 4 · From Origins to Frontier: A History of Stochastic Thermodynamics and Complex Systems

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Wmax⁡=kBTln⁡2W_{\max} = k_B T \ln 2

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Inputs and operationsk_B T ln 2
Result or conditionW_max
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Wmax⁡W_{\max}

Symbol W_max

WmW_max is part of the quantity the equation computes from the expression on the right.

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kBk_B

Symbol k_B

kBk_B is an input to the expression that computes the quantity on the left.

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TT

Symbol T

the bath temperature.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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What the article says around this equation

Szilard reduced Maxwell’s population of molecules to the simplest case that still carried the paradox: a single gas particle in a box. An external agent measures which half of the box the particle occupies, inserts a partition, and lets the particle push a piston on the side it occupies, converting the result of that one-bit measurement into extractable work. Szilard showed that the demon’s ability to extract work was tied exactly to the amount of information it acquired in the measurement — one bit of information corresponds to a definite quantity of work, kBk_B T ln⁡\ln 2 , where kBk_B is Boltzmann’s constant and T is the bath temperature. This is worth stating as an equation because it is the…
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Szilard reduced Maxwell’s population of molecules to the simplest case that still carried the paradox: a single gas particle in a box. An external agent measures which half of the box the particle occupies, inserts a partition, and lets the particle push a piston on the side it occupies, converting the result of that one-bit measurement into extractable work. Szilard showed that the demon’s ability to extract work was tied exactly to the amount of information it acquired in the measurement — one bit of information corresponds to a definite quantity of work, kBk_B T ln⁡\ln 2 , where kBk_B is Boltzmann’s constant and T is the bath temperature. This is worth stating as an equation because it is the single quantity that recurs across the rest of this history: Wmax⁡=kBTln⁡2W_{\max} = k_B T \ln 2. Szilard’s paper is a fact of the historical record: it is the first place a quantitative link between information and thermodynamic work appears in print. What it was not was a resolution of the paradox. Szilard asserted that the act of measurement itself must cost at least this much entropy somewhere else in the universe, closing the loop with the second law, but he did not derive that cost from a physical model of measurement — it was an assumption doing the work the physics had not yet earned. That gap between assertion and derivation would remain open for decades.

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