University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 26 - Direct-Current Circuits - Problems - Exercises - Page 873: 26.3

Answer

$P_t$ = 22.5 W

Work Step by Step

The voltage of the battery is the voltage across the resistance $R_1$, so we use the given values of $P_1$ to get the voltage of the battery as next \begin{gather*} P_{1} = \dfrac{V^{2}}{R_{1}} \\ \end{gather*} Solve for $V$ \begin{align*} V = \sqrt{P_{1}R_{1}} = \sqrt{(36 \,\text{W})(25 \mathrm{~\Omega})} = 30 \,\text{V} \end{align*} After $R_{2}$ is connected, the voltage drop in the battery will be due to the equivalent resistance which is calculated by $$ R_{eq} = R_{1} + R_{2} = 25 \mathrm{~\Omega} + 15 \mathrm{~\Omega} = 40 \mathrm{~\Omega} $$ The total dissipated power by the two resistors is calculated by \begin{gather*} P_{t} = \dfrac{V^{2}}{R_{eq}} \end{gather*} Substitute the values for $V, R_{1}$ and $R_{2}$to get the total dissipated power \begin{align*} P_{t} = \dfrac{V^{2}}{R_{eq}} = \dfrac{(30 \,\text{V})^{2}}{ 40 \mathrm{~\Omega} } = \boxed{22.5 \,\text{W}} \end{align*}  
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