Any reversible process can be described as a sum of many infinitesimally small Carnot cycles, so $\oint {dS} = \oint {\frac{{dQ}}{T}} = 0 % MathType!MTEF!2!1!+- % feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn % hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr % 4rNCHbWexLMBbXgBd9gzLbvyNv2CaeHb5MDXbpmVaibaieYlf9irVe % eu0dXdh9vqqj-hEeeu0xXdbba9frFj0-OqFfea0dXdd9vqaq-JfrVk % FHe9pgea0dXdar-Jb9hs0dXdbPYxe9vr0-vr0-vqpWqaaeaabiGaci % aacaqabeaadaqaaqaafaGcqaaaaaaaaaWdbeaadaWdfaqaaiaadsga % caWGtbaaleqabeqdcqWIr4E0cqGHRiI8aOGaeyypa0Zaa8qbaeaada % WcaaqaaiaadsgacaWGrbaabaGaamivaaaaaSqabeqaniablgH7rlab % gUIiYdGccqGH9aqpcaaIWaaaaa!5091! $ holds. It means the integral is independent of path it takes so the entropy S is a state variable. Such a path-independence is only true so reversible process, in strickly speaking. Then...is the entropy S not state variable for irreversible process?
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Entropy is a property of the system and it does not depend on the process that system experiences. Also, it does not depend on how you measure it. For irreversible process $\oint {\frac{{dQ}}{T}}$ is not equal to zero, but the system has a property called entropy at any instance that its change is depend only on initial and final states of the system.
lucas
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In an irreversible process, the system itself generates entropy that has to be added to the terms $\frac{\delta Q}{T}$ representing heat transfer from/to the outside. For example, if a current $I$ passes through a resistor $R$ at temperature $T$ the rate of entropy generation is $\frac{I^2R}{T}$ as measured in units of $\frac{joule}{kelvin \times sec}$.
hyportnex
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