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: 4-20

Answer

$W_{1-2} = 37.18\ kJ$ $W_{2-3} = -34.87\ kJ$ $W_{3-1} = -6.97\ kJ $ $W = -4.66\ kJ $

Work Step by Step

1-2) The work done is given by: $W = \frac{mRT_1}{M}\ln(\frac{P_1}{P_2})$ With: $m = 0.15\ kg,\ M=28.97\ kg/kmol,\ R=8.314\ kJ/kmol.K,\ T_1=350°C+273.15=623.15\ K$ $P_1 = 2\ MPa,\ P_2=500\ kPa$ We can get to: $W_{1-2} = 37.18\ kJ$ 2-3)For a polytropic process with an ideal gas: $\frac{T_3}{T_2}=(\frac{P_3}{P_2})^{\frac{n-1}{n}}$ With: $T_2 = T_1 = 623.15\ K, P_3 = P_1 = 2\ MPa,\ P_2 = 500\ kPa,\ n=1.2$ We have $T_3 = 785.12\ K$ The work done is given by: $W_{2-3} = \frac{mR}{M}\frac{(T_3-T_2)}{1-n}$ $W_{2-3} = -34.87\ kJ$ 3-1) The work done is: $W_{3-1} = P_3(V_1-V_3)=\frac{P_3mR}{M}(\frac{T_1}{P_1}-\frac{T_3}{P_3}) = \frac{mR}{M} (T_1-T_3)$ Therefore: $W_{3-1} = -6.97\ kJ $ Net work: $W = -4.66\ kJ $
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