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: 12-34

Answer

$u_{2}-u_{1}=205\text{ kJ/kg}$

Work Step by Step

Solving the equation of state for $P$ gives $$ P=\frac{R T}{v-a} $$ Then, $$ \left(\frac{\partial P}{\partial T}\right)_v=\frac{R}{v-a} $$ Using equation $12-29$, $$ d u=c_v d T+\left[T\left(\frac{\partial P}{\partial T}\right)_v-P\right] d v $$ Substituting, $$ \begin{aligned} d u & =c_v d T+\left(\frac{R T}{v-a}-\frac{R T}{v-a}\right) d v \\ & =c_v d T \end{aligned} $$ Integrating this result between the two states with constant specific heats gives $$ u_2-u_1=c_v\left(T_2-T_1\right)=(0.731 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(300-20) \mathrm{K}=\mathbf{2 0 5} \mathbf{k J} / \mathbf{k g} $$ The ideal gas model for the air gives $$ d u=c_\nu d T $$ which gives the same answer.
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