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: 26.4

Answer

(a) $13.5 \mathrm{~\Omega}$ (b) $17.7 \,\text{A}$ (c) $I_{1} = 5.7 \,\text{A}$ and $I_{2} = 12 \,\text{A}$

Work Step by Step

(a) The equivalent resistance of $R_{1}$ and $R_{2}$ which are in parallel is calculated by \begin{align*} R_{\text{eq}} = \dfrac{R_{1}R_{2}}{R_{1} + R_{2} } = \dfrac{(42 \mathrm{~\Omega})(20 \mathrm{~\Omega})}{42 \mathrm{~\Omega} + 20 \mathrm{~\Omega} } =\boxed{13.5 \mathrm{~\Omega}} \end{align*} (b) The voltage $V$ across resistors connected in parallel is the same and equals the potential difference across their combination. We use Ohm's law in the next form to get the current \begin{align*} I_{t} = \dfrac{V}{R_{\text{eq}}} = \dfrac{ 240 \,\text{V}}{13.5\mathrm{~\Omega}} = \boxed{17.7 \,\text{A}} \end{align*} (c) We mentioned in part (b) that the voltage is the same across the two resistors, so again we use Ohm's law to get the current in each resistor by \begin{align*} I_{1} = \dfrac{V}{R_{1}} = \dfrac{ 240 \,\text{V}}{42 \mathrm{~\Omega}} = \boxed{5.7 \,\text{A}} \end{align*} and, \begin{align*} I_{2} = \dfrac{V}{R_{2}} = \dfrac{ 240 \,\text{V}}{20 \mathrm{~\Omega}} = \boxed{12 \,\text{A}} \end{align*}
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