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 11 - Refrigeration Cycles - Problems - Page 646: 11-73

Answer

b) $ \operatorname{COP}_{\mathrm{R}}=0.525 $ c) $ \dot{m}=0.0791\text{ kg/s}$

Work Step by Step

(a) From the isentropic relations, $$ \begin{aligned} & T_{2 s}=T_1\left(\frac{P_2}{P_1}\right)^{(\mathrm{k}-1) / \mathrm{k}}=(267 \mathrm{~K})(4)^{0.667 / 1.667}=465.0 \mathrm{~K} \\ & T_{4 s}=T_3\left(\frac{P_4}{P_3}\right)^{(\mathrm{k}-1) / \mathrm{k}}=(323 \mathrm{~K})\left(\frac{1}{4}\right)^{0.667 / 1.667}=185.5 \mathrm{~K} \end{aligned} $$ and $$ \begin{aligned} & \begin{aligned} \eta_T=\frac{h_3-h_4}{h_3-h_{4 s}}=\frac{T_3-T_4}{T_3-T_{4 s}} \longrightarrow T_4 & =\\T_3-\eta_T\left(T_3-T_{4 s}\right)=323-(0.85)(323-185.5) & =\mathbf{2 0 6 . 1 ~ K}=T_{\min } \end{aligned} \\ & \begin{aligned} \eta_C=\frac{h_{2 s}-h_1}{h_2-h_1}=\frac{T_{2 s}-T_1}{T_2-T_1} \longrightarrow T_2 & \\=T_1+\left(T_{2 s}-T_1\right) / \eta_C=267+(465.0-267) /(0.85) & =499.9 \mathrm{~K} \end{aligned} \end{aligned} $$ (b) The COP of this gas refrigeration cycle is determined from $$ \begin{aligned} \operatorname{COP}_{\mathrm{R}} & =\frac{q_L}{w_{\text {net,in }}}=\frac{q_L}{w_{\text {comp, in }}-w_{\text {turbout }}} \\ & =\frac{h_1-h_4}{\left(h_2-h_1\right)-\left(h_3-h_4\right)} \\ & =\frac{T_1-T_4}{\left(T_2-T_1\right)-\left(T_3-T_4\right)} \\ & =\frac{267-206.1}{(499.9-267)-(323-206.1)} \\ & =\mathbf{0 . 5 2 5} \end{aligned} $$ (c) The mass flow rate of helium is determined from $$ \dot{m}=\frac{\dot{Q}_{\text {refig }}}{q_L}=\frac{\dot{Q}_{\text {refig }}}{h_1-h_4}=\frac{\dot{Q}_{\text {refig }}}{c_p\left(T_1-T_4\right)}=\frac{25 \mathrm{~kJ} / \mathrm{s}}{(5.1926 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K})(267-206.1) \mathrm{K}}=0.0791 \mathrm{~kg} / \mathrm{s} $$
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