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 649: 11-111

Answer

a) $T_2=54.5^{\circ}C$ b) $\dot{Q}_{\text {people }}=0.665\text{ kW}$ c) $COP_{}=5.87$ d) $ \dot{V}_{1, \min }=15.7\text{ L/min}$

Work Step by Step

(a) From the refrigerant-134a tables (Tables A-11 through A-13) $$ \begin{aligned} & \left.\begin{array}{l} P_1=500\ \mathrm{kPa} \\ x_1=1 \end{array}\right\} \begin{array}{l} h_1=259.36 \mathrm{~kJ} / \mathrm{kg} \\ v_1=0.04117 \mathrm{~kJ} / \mathrm{kg} \\ s_1=0.9242 \mathrm{~kJ} / \mathrm{kg} \end{array} \\ & \left.\begin{array}{l} P_2=1200\ \mathrm{kPa} \\ s_2=s_1 \end{array}\right\} h_{2 s}=277.45 \\ & h_3=h_{f @ 1200 \mathrm{kPa}}=117.79 \mathrm{~kJ} / \mathrm{kg} \\ & h_4=h_3=117.79 \mathrm{~kJ} / \mathrm{kg} \\ & \eta_C=\frac{h_{2 s}-h_1}{h_2-h_1} \\ & 0.75=\frac{277.45-259.36}{h_2-259.36} \longrightarrow h_2=283.48 \mathrm{~kJ} / \mathrm{kg} \\ & \left.\begin{array}{l} P_2=1200\ \mathrm{kPa} \\ h_2=283.48 \mathrm{~kJ} / \mathrm{kg} \end{array}\right\} T_2=\mathbf{5 4 . 5}^{\circ} \mathrm{C} \end{aligned} $$ (b) The mass flow rate of the refrigerant is $$ \dot{m}=\frac{\dot{V}_1}{v_1}=\frac{(100 \mathrm{~L} / \mathrm{min})\left(\frac{1 \mathrm{~m}^3}{1000 \mathrm{~L}}\right)\left(\frac{1 \mathrm{~min}}{60 \mathrm{~s}}\right)}{0.04117 \mathrm{~m}^3 / \mathrm{kg}}=0.04048 \mathrm{~kg} / \mathrm{s} $$ The refrigeration load is $$ \dot{Q}_L=\dot{m}\left(h_1-h_4\right)=(0.04048 \mathrm{~kg} / \mathrm{s})(259.36-117.79) \mathrm{kJ} / \mathrm{kg}=5.731 \mathrm{~kW} $$ which is the total heat removed from the room. Then, the rate of heat generated by the people in the room is determined from $$ \dot{Q}_{\text {people }}=\dot{Q}_L-\dot{Q}_{\text {heat }}-\dot{Q}_{\text {equip }}=(5.731-250 / 60-0.9) \mathrm{kW}=\mathbf{0 . 6 6 5 k W} $$ (c) The power input and the COP are $$ \begin{aligned} & \dot{W}_{\text {in }}=\dot{m}\left(h_2-h_1\right)=(0.04048 \mathrm{~kg} / \mathrm{s})(283.48-259.36) \mathrm{kJ} / \mathrm{kg}=0.9764 \mathrm{~kW} \\ & \mathrm{COP}=\frac{\dot{Q}_{\mathrm{L}}}{\dot{W}_{\text {in }}}=\frac{5.731}{0.9764}=\mathbf{5 . 8 7} \end{aligned} $$ (d) The reversible COP of the cycle is $$ \mathrm{COP}_{\mathrm{nev}}=\frac{1}{T_H / T_L-1}=\frac{1}{(34+273) /(26+273)-1}=37.38 $$ The corresponding minimum power input is $$ \dot{W}_{\mathrm{in}, \min }=\frac{\dot{Q}_{\mathrm{L}}}{\operatorname{COP}_{\mathrm{rev}}}=\frac{5.731 \mathrm{~kW}}{37.38}=0.1533 \mathrm{~kW} $$ The minimum mass and volume flow rates are $$ \begin{aligned} & \dot{m}_{\min }=\frac{\dot{W}_{\text {in,min }}}{h_2-h_1}=\frac{0.1533 \mathrm{~kW}}{(283.48-259.36) \mathrm{kJ} / \mathrm{kg}}=0.006358 \mathrm{~kg} / \mathrm{s} \\ & \dot{V}_{1, \min }=\dot{m}_{\min } \nu_1=(0.006358 \mathrm{~kg} / \mathrm{s})\left(0.04117 \mathrm{~m}^3 / \mathrm{kg}\right)=\left(0.0002618 \mathrm{~m}^3 / \mathrm{s}\right)=15.7 \mathrm{L/min} \end{aligned} $$
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