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 200: 4-56E

Answer

$\Delta u=78.41\ Btu/lbm$ $\Delta h=110.67\ Btu/lbm$

Work Step by Step

The circular profile of the 10 in diameter piston has an area of: $A=\frac{\pi}{4}D^2 = 0.545\ ft²$ Hence the initial height of 1 ft³ of air is: $V=A.x \rightarrow x_0= 1.833\ ft$ Since the final volume is half of the original: $x_1 = 0.9167\ ft$, and $\Delta x = -0.9167\ ft = -11\ in$ With a spring constant of $k = 5\ lbf/in$, the elastic force is $F=-55\ lbf$ and $\Delta P = F/A= -0.70\ psia$ Thus, the final pressure is: $P_2=249.3\ psia$ From the ideal gas relation ($T_1=460°F=919.67°R, R=0.3704\ psia.ft³/lbm.°R$): $PV=mRT$ The mass is $m=0.7339\ lbm$ Therefore the final temperature is: $T_2=458.55°R$ From table A-2a $c_{p,\ avg}\approx c_{p,\ 80°F} = 0.240\ Btu/lbm.°R$: So: $\Delta h=c_p\Delta T$ $\Delta h=110.67\ Btu/lbm$ $c_{v,\ avg}\approx c_{v,\ 80°F} = 0.171\ Btu/lbm.°R$: $\Delta u=c_v\Delta T$ $\Delta u=78.41\ Btu/lbm$
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