Thermodynamics: An Engineering Approach 8th Edition

Published by McGraw-Hill Education
ISBN 10: 0-07339-817-9
ISBN 13: 978-0-07339-817-4

Chapter 9 - Gas Power Cycles - Problems - Page 539: 9-19

Answer

$P_{1}=6524\text{ kPa}$ $Q_{in}=0.706\text{ kJ}$ $m=0.000409\text{ kg}$

Work Step by Step

(a) In a Carnot cycle, the maximum pressure occurs at the beginning of the expansion process, which is state 1 $$ \frac{T_1}{T_4}=\left(\frac{P_1}{P_4}\right)^{(k-1) / k} $$ or, $$ P_1=P_4\left(\frac{T_1}{T_4}\right)^{k /(k-1)}=(300 \mathrm{kPa})\left(\frac{1200 \mathrm{~K}}{350 \mathrm{~K}}\right)^{1.667 / 0.66}=\mathbf{6 5 2 4} \mathbf{~ k P a} $$ (b) The heat input is determined from $$ \begin{aligned} & \eta_{\text {th }}=1-\frac{T_L}{T_H}=1-\frac{350 \mathrm{~K}}{1200 \mathrm{~K}}=70.83 \% \\ & Q_{\text {in }}=W_{\text {net,out }} / \eta_{\text {th }}=(0.5 \mathrm{~kJ}) /(0.7083)=\mathbf{0 . 7 0 6}\ \mathbf{k J} \end{aligned} $$ (c) The mass of helium is determined from $$ \begin{aligned} s_4-s_3 & =c_p \ln {\frac{T_4}{T_3}}^{\circ 0}-R \ln \frac{P_4}{P_3}=-(2.0769 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}) \ln \frac{300 \mathrm{kPa}}{150 \mathrm{kPa}} \\ & =-1.4396 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}=s_1-s_2 \\ w_{\text {net,out }} & =\left(s_2-s_1\right)\left(T_H-T_L\right)=(1.4396 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(1200-350) \mathrm{K}=1223.7 \mathrm{~kJ} /kg \\ m & =\frac{W_{\text {net,out }}}{w_{\text {net,out }}}=\frac{0.5 \mathrm{~kJ}}{1223.7 \mathrm{~kJ} / \mathrm{kg}}=\mathbf{0 . 0 0 0 4 0 9}\ \mathbf{k g} \end{aligned} $$
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