Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 15 - The Laws of Thermodynamics - General Problems - Page 441: 70

Answer

a) $ { 4.76}^\circ \rm C$ b) $69.3\;\rm J/kg.K$

Work Step by Step

a) We need to find the rate of exhausted heat to the river, so we can find the change in temperature. $$Q_{river}^+=Q_L=mc\Delta T$$ whereas $Q_{river}^+$ is the amount of heat absorbed by the water of the river which is the amount of heat $Q_L$ exhausted from the power plant. Dividing both sides by $t$; $$\dfrac{Q_L}{t}=\dfrac{m_{river} c_{river}\Delta T_{river}}{t}$$ We also know, from the density law, that $m=\rho V$ So that, $$\dfrac{Q_L}{t}=\dfrac{\rho_{river} V_{river} c_{river}\Delta T_{river}}{t}$$ $$ \dfrac{Q_L}{t}=\rho_{river} c_{river}\Delta T_{river}\dfrac{V_{river}}{t}\tag 1$$ And since the author assumed that the turbine operates as an ideal Carnot engine, so $$e= \dfrac{T_H-T_L}{T_H}=\dfrac{W}{Q_H}=\dfrac{W}{W+Q_L}$$ Thus, $$ \dfrac{T_H-T_L}{T_H} =\dfrac{W}{W+Q_L}$$ Solving for $Q_L$; $$T_HW=(T_H-T_L)(W+Q_L)$$ $$W+Q_L=\dfrac{T_HW}{T_H-T_L}$$ $$ Q_L=\dfrac{T_HW}{T_H-T_L}-W=W\left(\dfrac{T_H }{T_H-T_L}-1\right)$$ Dividing both sides by $t$; $$ \dfrac{Q_L}{t}= \overbrace{ \left[\dfrac{W}{t} \right]}^{ P}\left(\dfrac{T_H }{T_H-T_L}-1\right)\tag 2$$ From (1) and (2); $$ \rho_{river} c_{river}\Delta T_{river}\dfrac{V_{river}}{t}=P\left(\dfrac{T_H }{T_H-T_L}-1\right) $$ Plugging the known and solving for $\Delta T$; $$ 1000\cdot 4186\cdot 37 \Delta T_{river} =880 \times 10^6 \left(\dfrac{625}{625-285}-1\right) $$ Thus, $$\Delta T=\color{red}{\bf 4.76}\;\rm K=\color{red}{\bf 4.76}^\circ C$$ b) Now we need to find the entropy increase per kilogram of the water of the river. $$\dfrac{\Delta S}{m}=\dfrac{Q}{T}=\dfrac{mc\Delta T}{mT}$$ Thus, $$\dfrac{\Delta S}{m}=\dfrac{c\Delta T}{T_{avg}}\tag 3$$ whereas $T_{avg}$ is the average temperature of the water which is given by $$T_{avg}=\dfrac{T_f+T_i}{2}=\dfrac{T_i+\Delta T+T_i}{2}$$ Plugging the know; $$T_{avg}=\dfrac{2T_i+\Delta T }{2}=\dfrac{(2\cdot 285)+ 4.76}{2}=\bf 287.4 \;\rm K $$ Plugging into (3) and plug the known as well; $$\dfrac{\Delta S}{m}=\dfrac{4186\cdot 4.76}{287.4 } $$ $$\dfrac{\Delta S}{m}=\color{red}{\bf 69.3}\;\rm J/kg.K$$
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