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: 9-86

Answer

$r_{\mathrm{bw}}=0.8387$

Work Step by Step

For the compression process, $$ \begin{aligned} T_{2 s}=T_1\left(\frac{P_2}{P_1}\right)^{(k-1) / k}=(288 \mathrm{~K})(12)^{0.4 / 1.4} & =585.8 \mathrm{~K} \\ \eta_C=\frac{h_{2 s}-h_1}{h_2-h_1}=\frac{c_p\left(T_{2 s}-T_1\right)}{c_p\left(T_2-T_1\right)} \longrightarrow T_2 & =T_1+\frac{T_{2 s}-T_1}{\eta_C} \\ & =288+\frac{585.8-288}{0.80} \\ & =660.2 \mathrm{~K} \end{aligned} $$ For the expansion process, $$ \begin{aligned} T_{4 s}=T_3\left(\frac{P_4}{P_3}\right)^{(k-1) / k}=(873 \mathrm{~K})\left(\frac{1}{12}\right)^{0.4 / 1.4} & =429.2 \mathrm{~K} \\ \eta_T=\frac{h_3-h_4}{h_3-h_{4 s}}=\frac{c_p\left(T_3-T_4\right)}{c_p\left(T_3-T_{4 s}\right)} \longrightarrow T_4 & =T_3-\eta_T\left(T_3-T_{4 s}\right) \\ & =873-(0.80)(873-429.2) \\ & =518.0 \mathrm{~K} \end{aligned} $$ The isentropic and actual work of compressor and turbine are $$ \begin{aligned} & W_{\text {Comp}, s}=c_p\left(T_{2 s}-T_1\right)=(1.005 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(585.8-288) \mathrm{K}=299.3 \mathrm{~kJ} / \mathrm{kg} \\ & W_{\text {Comp }}=c_p\left(T_2-T_1\right)=(1.005 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(660.2-288) \mathrm{K}=374.1 \mathrm{~kJ} / \mathrm{kg} \\ & W_{\text {Turb, } s}=c_p\left(T_3-T_{4 s}\right)=(1.005 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(873-429.2) \mathrm{K}=446.0 \mathrm{~kJ} / \mathrm{kg} \\ & W_{\text {Turb }}=c_p\left(T_3-T_4\right)=(1.005 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(873-518.0) \mathrm{K}=356.8 \mathrm{~kJ} / \mathrm{kg} \end{aligned} $$ The back work ratio for $90 \%$ efficient compressor and isentropic turbine case is $$ r_{\text {bw }}=\frac{W_{\text {Comp }}}{W_{\text {Tub }, s}}=\frac{374.1 \mathrm{~kJ} / \mathrm{kg}}{446.0 \mathrm{~kJ} / \mathrm{kg}}=\mathbf{0 . 8 3 8 7} $$ The back work ratio for $90 \%$ efficient turbine and isentropic compressor case is $$ r_{\mathrm{bw}}=\frac{W_{\text {Comp }, s}}{W_{\text {Turb }}}=\frac{299.3 \mathrm{~kJ} / \mathrm{kg}}{356.8 \mathrm{~kJ} / \mathrm{kg}}=\mathbf{0 . 8 3 8 7} $$ The two results are identical.
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.