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 641: 11-22

Answer

c) $178.5\text{ kJ/kg}$

Work Step by Step

(a) In this normal vapor-compression refrigeration cycle, the refrigerant enters the compressor as a saturated vapor at the evaporator pressure, and leaves the condenser as saturated liquid at the condenser pressure. (b) $$ \begin{aligned} & h_4=h_3=h_{f @45{ }^{\circ}C}=101 \mathrm{~kJ} / \mathrm{kg} \\ & h_1=h_{g@-5^{\circ}\mathrm{C}}=248.1 \mathrm{~kJ} / \mathrm{kg} . \end{aligned} $$ The heat absorbed by the refrigerant in the evaporator is $$ q_L=h_1-h_4=248.1-101=147.1 \mathrm{~kJ} / \mathrm{kg} $$ (c) The COP of the air conditioner is $$ \operatorname{COP}_{\mathrm{R}}=\operatorname{SEER}\left(\frac{1 \mathrm{~W}}{3.412 \mathrm{Btu} / \mathrm{h}}\right)=\left(16 \frac{\mathrm{Btu} / \mathrm{h}}{\mathrm{W}}\right)\left(\frac{1 \mathrm{~W}}{3.412 \mathrm{Btw} / \mathrm{h}}\right)=4.689 $$ The work input to the compressor is $$ \mathrm{COP}_{\mathrm{R}}=\frac{q_L}{w_{\text {in }}} \longrightarrow w_{\text {in }}=\frac{q_L}{\mathrm{COP}_{\mathrm{R}}}=\frac{147.1 \mathrm{~kJ} / \mathrm{kg}}{4.689}=31.4 \mathrm{~kJ} / \mathrm{kg} $$ The enthalpy at the compressor exit is $$ w_{\text {in }}=h_2-h_1 \longrightarrow h_2=h_1+w_{\text {in }}=248.1 \mathrm{~kJ} / \mathrm{kg}+31.4 \mathrm{~kJ} / \mathrm{kg}=279.5 \mathrm{~kJ} / \mathrm{kg} $$ The heat rejected from the refrigerant in the condenser is then $$ q_H=h_2-h_3=279.5-101=178.5 \mathrm{~kJ} / \mathrm{kg} $$
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