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: 4-15

Answer

a)$[10] = \frac{m^6.kPa}{kmol^2}$ b)$W = 403.3\ kJ$

Work Step by Step

a) The left-hand side of the equation expands to: $\bar{v}P + 10/\bar{v}$, therefore these two terms must have the same units to make the addition operation possible. $(m³/kmol).kPa = \frac{[10]}{m³/kmol}$ $[10] = \frac{m^6.kPa}{kmol^2}$ b) Re-arranging the equation of state we get to: $P = \frac{R_uT}{\bar{v}}-\frac{10}{\bar{v}^2}$ $P = \frac{nR_uT}{V}-\frac{10n^2}{V^2}$ With the work equation being: $W = \int PdV$ $W = \int_{2\ m³}^{4\ m³} \frac{nR_uT}{V}-\frac{10n^2}{V^2} dV$ $W = (nR_uT\ln(V) +\frac{10n^2}{V})|_{2\ m³}^{4\ m³}$ Given the values of: $n = 0.2\ kmol,\ R_u=8.314kJ/kmol.K,\ T=350K$ $W = 403.3\ kJ$
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