Show that in a reversible engine the amount of heat \(Q_{C}\) exhausted to the cold reservoir is related to the net work done \(W_{\text {net }}\) by $$ Q_{\mathrm{C}}=\frac{T_{\mathrm{C}}}{T_{\mathrm{H}}-T_{\mathrm{C}}} W_{\mathrm{net}} $$

Short Answer

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Answer: The amount of heat exhausted to the cold reservoir \(Q_C\) is related to the net work done \(W_{\text{net}}\) by the equation: $$ Q_{\mathrm{C}}=\frac{T_{\mathrm{C}}}{T_{\mathrm{H}}-T_{\mathrm{C}}}W_{\mathrm{net}} $$

Step by step solution

01

Efficiency for Reversible Engines

A reversible engine operating between hot and cold reservoirs is the most efficient engine possible. Its efficiency is given by: $$ \eta_{\text{rev}} = 1 - \frac{T_C}{T_H} $$
02

Relating Heat and Work Transfer to Efficiency

Since the efficiency of an engine is defined as the ratio of the work done to the heat absorbed from the hot reservoir, we can write: $$ \eta_{\text{rev}} = \frac{W_{\text{net}}}{Q_H} $$ Then, we substitute the expression for the efficiency from Step 1: $$ 1 - \frac{T_C}{T_H} = \frac{W_{\text{net}}}{Q_H} $$
03

Heat Transfer to Cold Reservoir

In a reversible engine, the relationship between heat absorbed from the hot reservoir \(Q_H\) and heat exhausted to the cold reservoir \(Q_C\) is: $$ Q_H = Q_C + W_{\text{net}} $$
04

Substituting and Solving for \(Q_C\)

Now, we can substitute the expression for \(Q_H\) from Step 3 into the equation from Step 2: $$ 1 - \frac{T_C}{T_H} = \frac{W_{\text{net}}}{Q_C + W_{\text{net}}} $$ Then, we can solve for \(Q_C\): $$ Q_C\left(1 - \frac{T_C}{T_H}\right) = W_{\text{net}} - \frac{T_C}{T_H}W_{\text{net}} $$ $$ Q_C =\frac{T_C}{T_H - T_C} W_{\text{net}} $$
05

Conclusion

We have shown that, for a reversible engine, the amount of heat exhausted to the cold reservoir \(Q_C\) is related to the net work done \(W_{\text{net}}\) by the given equation: $$ Q_{\mathrm{C}}=\frac{T_{\mathrm{C}}}{T_{\mathrm{H}}-T_{\mathrm{C}}}W_{\mathrm{net}} $$

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