Subjective Type

The conditions are the same as in the foregoing problem with the exception that the isothermal process proceeds at the maximum temperature of the whole cycle.

Solution

Here the isothermal process proceeds at the maximum temperature instead of at the minimum temperature of the cycle.
(a) Here $$p_1 V_1 = p_0V_0, p_2 = \frac{p_1}{n}$$
$$p_2V_2^{\gamma} = p_0V_0^{\gamma}$$ or $$ p_1V_1^{\gamma} = np_0 V_0^{\gamma}$$
i.e., $$V_1^{\gamma -1} = nV_0^{\gamma -1}$$ or $$V_1 = V_0 n^{\frac{1}{\gamma -1}}$$
$$Q_2' = C_VT_0\Big( 1 - \frac{1}{n}\Big), Q_1 = RT_0 In \frac{V_1}{V_0}= \frac{RT_0}{\gamma - 1}In \ n = C_V T_0 In \ n$$.
Thus $$\eta = 1 - \frac{Q_2'}{Q_1} = 1 - \frac{n-1}{n \ In \ n}$$
(b) Here $$ V_2 = \frac{V_1}{n} , \ p_0V_0 = p_1V_1$$
$$p_0V_0^{\gamma} = p_1V_2^{\gamma} = p_1 n^{-\gamma}V_1^{\gamma} =V_0^{\gamma -1} n^{-\gamma} V_1^{\gamma -1}$$ or $$V_1 = n^{(\gamma / \gamma -1)} V_0$$
$$Q_2' = C_pT_0\Big(1 - frac{1}{n}\Big)$$, $$Q_1 = RT_0 \ In \ \frac{V_1}{V_0} = \frac{R\gamma}{\gamma -1} T_0 \ In \ n = C_pT_0 \ In \ n$$
Thus $$\eta = 1 - \frac{n-1}{n \ In \ n}$$


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