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Chjoaygame (talk | contribs) →Thermodynamic entropy: wording |
Chjoaygame (talk | contribs) →Thermodynamic entropy: wording |
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Thermodynamic entropy is only measured as a change in entropy (<math>\Delta S</math>) to a system containing a sub-system which undergoes heat transfer to its surroundings (inside the system of interest). It is based on the [[macroscopic]] relationship between [[heat flow]] into the sub-system and the temperature at which it occurs summed over the boundary of that sub-system.
Following the [[Clausius theorem|formalism of Clausius]], the
: <math>{\rm \delta}S = \frac{{\rm \delta}q}{T}.</math>
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: <math>{{\rm \delta}S} \ge {\frac{{\rm \delta}q}{T}}.</math>
According to the [[first law of thermodynamics]], which deals with the [[conservation of energy]], the loss <math>\delta q</math> of heat will result in a decrease in the [[internal energy]] of the [[thermodynamic system]]. Thermodynamic entropy provides a comparative measure of the amount of decrease in internal energy and the corresponding increase in internal energy of the surroundings at a given temperature. In many cases, a visualization of the second law is that energy of all types changes from being localized to becoming dispersed or spread out, if it is not hindered from doing so. When applicable, entropy
===Statistical mechanics and information entropy===
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