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 9 - Gas Power Cycles - Problems - Page 542: 9-80E

Answer

$r_{\mathrm{bw}}=48.5\%$ $ \eta_{\text {th }}=46.5\%$

Work Step by Step

(a) Noting that process 1-2 is isentropic, $$ \begin{aligned} & T_1=520\ \mathrm{R} \longrightarrow \begin{array}{l} h_1=124.27\ \mathrm{Btu} / \mathrm{lbm} \\ P_{r_1}=1.2147 \end{array} \\ & P_{r_2}=\frac{P_2}{P_1} P_{r_1}=(10)(1.2147)=12.147 \longrightarrow \begin{array}{l} T_2=996.5\ \mathbf{R} \\ h_2=240.11\ \mathrm{Btu} / \mathrm{lbm} \end{array} \end{aligned} $$ (b) Process 3-4 is isentropic, and thus $$ \begin{aligned} T_3 & =2000\ \mathrm{R} \longrightarrow \begin{array}{l} h_3=504.71\ \mathrm{Btu} / \mathrm{lbm} \\ P_{r_3}=174.0 \end{array} \\ P_{r_4} & =\frac{P_4}{P_3} P_{r_3}=\left(\frac{1}{10}\right)(174.0)=17.4 \longrightarrow h_4=265.83\ \mathrm{Btu} / \mathrm{lbm} \\ w_{\mathrm{C}, \text { in }} & =h_2-h_1=240.11-124.27=115.84\ \mathrm{Btu} / \mathrm{lbm} \\ w_{\mathrm{T}, \text { out }} & =h_3-h_4=504.71-265.83=238.88\ \mathrm{Btu} / \mathrm{lbm} \end{aligned} $$ Then the back-work ratio becomes $$ r_{\mathrm{bw}}=\frac{w_{\mathrm{C}, \text { in }}}{w_{\mathrm{T}, \text { out }}}=\frac{115.84 \mathrm{Btu} / \mathrm{lbm}}{238.88 \mathrm{Btu} / \mathrm{lbm}}=\mathbf{4 8 . 5} \% $$ (c) $$ \begin{aligned} & q_{\text {in }}=h_3-h_2=504.71-240.11=264.60\ \mathrm{Btu} / \mathrm{lbm} \\ & w_{\text {net,out }}=w_{\mathrm{T}, \text { out }}-w_{\mathrm{C}, \text { in }}=238.88-115.84=123.04\ \mathrm{Btu} / \mathrm{lbm} \\ & \eta_{\text {th }}=\frac{w_{\text {net,out }}}{q_{\text {in }}}=\frac{123.04 \mathrm{Btu} / \mathrm{lbm}}{264.60 \mathrm{Btu} / \mathrm{lbm}}=46.5 \% \end{aligned} $$
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