LTP
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Is it possible to show that the maximum efficiency for a heat engine is given by
\eta = 1 - \frac{T_c}{T_h}
where T_c is the temperature of the cold sink and T_c is the temperature of the warm sink?
In other words: How do I prove that a engine run by a Carnot cycle is the most efficient engine?
\eta = 1 - \frac{T_c}{T_h}
where T_c is the temperature of the cold sink and T_c is the temperature of the warm sink?
In other words: How do I prove that a engine run by a Carnot cycle is the most efficient engine?