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: 4-14

Answer

$W = -408.43\ kJ$

Work Step by Step

Assuming ideal gas behaviour: $P_1V_1 = \frac{m}{M}RT_1$ Given the values: $P_1 = 100\ kPa,\ m=5\ kg,\ M=28.014\ kg/kmol,\ R=8.314\ kJ/K.kmol,\ T_1=250\ K$ We can calculate $V_1 = 3.71\ m³$ For the polytropic process $PV^{1.4}=c$, we can calculate $c = 626.792\ kPa.m^{4.2}$ For the second state: $P_2V_2 = \frac{m}{M}RT_2$ Since $V_2 = V_2^{1.4}V_2^{-0.4}$ and $P_2V_2^{1.4} = c$ $cV_2^{-0.4} = \frac{m}{M}RT_2$ Knowing $T_2 = 360K$ we can calculate: $V_2 = 1.49\ m³,\ P_2 = 358.64\ kPa $ From the polytropic work expression: $W = \frac{P_2V_2-P_1V_1}{1-n}$ $W = -408.43\ kJ$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.