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 651: 11-124

Answer

$\mathrm{COP}_{\mathrm{R}}=4.62$

Work Step by Step

From the refrigerant tables (Tables A-11, A-12, and A-13), $$ \begin{aligned} & \left.\begin{array}{l} \begin{array}{l} P_3=900\ \mathrm{kPa} \\ \text { sat. liquid } \end{array} \end{array}\right\} h_3=h_{f @ 900 \mathrm{kPa}}=101.62 \mathrm{~kJ} / \mathrm{kg} \\ & \left.\begin{array}{rl} T_4 & =T_{\text {sat } @ 900 \mathrm{kPa}}-9.51 \\ & =35.51-9.51=26^{\circ} \mathrm{C} \\ P_4 & =900 \mathrm{kPa} \end{array}\right\} h_4 \equiv h_{f @ 26^{\circ} \mathrm{C}}=87.82 \mathrm{~kJ} / \mathrm{kg} \\ & h_5 \equiv h_4=87.82 \mathrm{~kJ} / \mathrm{kg} \quad \text { (throttling) } \\ & \left.T_6=-10.09^{\circ} \mathrm{C}\right\} \quad h_6=h_{g @-10.09^{\circ} \mathrm{C}}=244.50 \mathrm{~kJ} / \mathrm{kg} \\ & \text { sat. vapor }\} P_6=P_{\text {sat }@-10.09 \mathrm{C}}=200\ \mathrm{kPa} \end{aligned} $$ An energy balance on the heat exchanger gives $$ \dot{m}\left(h_1-h_6\right)=\dot{m}\left(h_3-h_4\right) \longrightarrow h_1=h_3-h_4+h_6=101.62-87.82+244.50=258.29 \mathrm{~kJ} / \mathrm{kg} $$ Then, $$ \begin{aligned} & \left.\begin{array}{l} P_1=200\ \mathrm{kPa} \\ h_1=258.29 \mathrm{~kJ} / \mathrm{kg} \end{array}\right\} s_1=0.9888 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K} \\ & \left.\begin{array}{l} P_2=900\ \mathrm{kPa} \\ s_2=s_1 \end{array}\right\} h_2=292.19 \mathrm{~kJ} / \mathrm{kg} \end{aligned} $$ The COP of this refrigeration system is determined from its definition, $$ \mathrm{COP}_{\mathrm{R}}=\frac{q_L}{w_{\text {in }}}=\frac{h_6-h_5}{h_2-h_1}=\frac{244.50-87.82}{292.19-258.29}=\mathbf{4 . 6 2} $$
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