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 12 - Thermodynamic Property Relations - Problems - Page 681: 12-39

Answer

$s_{2}-s_{1}=−0.2386\text{ kJ/kg⋅K}$

Work Step by Step

Solving the equation of state for $v$ gives $$ v=\frac{R T}{P}+a $$ Then, $$ \left(\frac{\partial v}{\partial T}\right)_P=\frac{R}{P} $$ The entropy differential is $$ \begin{aligned} d s & =c_p \frac{d T}{T}-\left(\frac{\partial v}{\partial T}\right)_P d P \\ & =c_p \frac{d T}{T}-R \frac{d P}{P} \end{aligned} $$ which is the same as that of an ideal gas. Integrating this result between the two states gives $$ \begin{aligned} s_2-s_1 & =c_p \ln \frac{T_2}{T_1}-R \ln \frac{P_2}{P_1} \\ & =(5.1926 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}) \ln \frac{573 \mathrm{~K}}{293 \mathrm{~K}}-(2.0769 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}) \ln \frac{600 \mathrm{kPa}}{100 \mathrm{kPa}} \\ & =-0.2386 \mathrm{~kJ} / \mathbf{k g} \cdot \mathbf{K} \end{aligned} $$
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