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 542: 9-74

Answer

$q_{in}=1275\text{ kJ/kg}$ $q_{out}=212.5\text{ kJ/kg}$ $w_{net}=1063\text{ kJ/kg}$

Work Step by Step

Applying the ideal gas equation to the isothermal process 3-4 gives $$ P_4=P_3 \frac{\boldsymbol{v}_3}{\boldsymbol{v}_4}=(50 \mathrm{kPa})(12)=600\ \mathrm{kPa} $$ Since process 4-1 is one of constant volume, $$ T_1=T_4\left(\frac{P_1}{P_4}\right)=(298 \mathrm{~K})\left(\frac{3600 \mathrm{kPa}}{600 \mathrm{kPa}}\right)=1788 \mathrm{~K} $$ Adapting the first law and work integral to the heat addition process gives $$ q_{\text {in }}=w_{1-2}=R T_1 \ln \frac{\boldsymbol{v}_2}{\boldsymbol{v}_1}=(0.287 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(1788 \mathrm{~K}) \ln (12)=\mathbf{1 2 7 5}\ \mathbf{k J} / \mathbf{k g} $$ Similarly, $$ q_{\text {out }}=w_{3-4}=R T_3 \ln \frac{\boldsymbol{v}_4}{\boldsymbol{v}_3}=(0.287 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(298 \mathrm{~K}) \ln \left(\frac{1}{12}\right)=\mathbf{2 1 2 . 5}\ \mathrm{kJ} / \mathbf{k g} $$ The net work is then $$ w_{\text {net }}=q_{\text {in }}-q_{\text {out }}=1275-212.5=\mathbf{1 0 6 3 ~k J / k g} $$
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