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 4 - Energy Analysis of Closed Systems - Problems - Page 197: 4-23

Answer

b) $\omega = \frac{-W_{1-2}}{W_{2-3}}= \frac{1}{n-1}\frac{1-r^{1-n}}{r-1}$ c) $\omega = 0.2558$

Work Step by Step

a) Process 1-2 is defined by the hyperbolic equation $PV^n=c$ in the P-V diagram, whereas process 2-3 is a straight horizontal line. b)For the polytropic process: $W_{1-2} = \frac{P_1V_1-P_2V_2}{n-1} $ $W_{1-2} = (\frac{P_2V_2}{n-1}) (\frac{P_1V_1}{P_2V_2}-1)$ With: $P_1V_1^n=P_2V_2^n \Rightarrow \frac{P_1}{P_2} = r^{-n} $ $W_{1-2} = (\frac{P_2V_2}{n-1}) (r^{1-n}-1)$ For the isobaric process: $W_{2-3} = P_2(V_3-V_2)$, With $V_3=V_1$ $W_{2-3} = P_2V_2(r-1)$ The rate $\omega = \frac{-W_{1-2}}{W_{2-3}}$ $\omega = \frac{1}{n-1}\frac{1-r^{1-n}}{r-1}$ c) With n=1.4 and r=6: $\omega = 0.2558$
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