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 874: 26.9

Answer

(a) $8.8 \mathrm{~\Omega}$ (b) 3.18 A (c) 3.18 A (d) $V_{1.6} = 5.09 \,\text{V}, V_{2.4} = 7.63 \,\text{V}, V_{4.8} = 15.26 \,\text{V} $ (e) $P_{1.6} = 16.18 \,\text{W}, P_{2.4} =24.27 \,\text{W}, P_{4.8} = 48.54 \,\text{W}$ (f) Greatest resistance

Work Step by Step

\subsection*{Solution} (a) The equivalent resistance for the three reistsors in series is given by \begin{align*} R_{eq}& = 1.6 \mathrm{~\Omega} + 2.4 \mathrm{~\Omega} +4.8 \mathrm{~\Omega}\\ & = \boxed{8.8 \mathrm{~\Omega}} \end{align*} (b) The current is the same for the resistors in series and from Ohm's law we get the current by $$I_{1.6} = I _{2.4} = I_{4.8 } = I$$ And from Ohm's law, we could calculate the current for the combination $I$ by \begin{align*} I = I_{1.6} = I _{2.4} = I_{4.8 }= \dfrac{V}{R_{eq}} = \dfrac{28.0 \,\text{V}}{8.8 \mathrm{~\Omega}} = \boxed{3.18 \,\text{A}} \end{align*} (c) The battery has the same current as it is in series with the resistors \begin{align*} I = \boxed{3.18 \,\text{A} } \end{align*} (d) Each resistor in series has its own voltage with the same current, so for each resistor the voltage is \begin{gather*} V_{1.6} = IR_{1.6} =(3.18 \,\text{A})(1.6 \mathrm{~\Omega}) = \boxed{5.09 \,\text{V}}\\ V_{2.4} = IR_{2.4} =(3.18 \,\text{A})(2.4 \mathrm{~\Omega}) = \boxed{7.63 \,\text{V}}\\ V_{4.8} = IR_{4.8 } =(3.18 \,\text{A})(4.8 \mathrm{~\Omega}) = \boxed{15.26 \,\text{V}} \end{gather*} (e) The dissipated power in each resistor is given by \begin{gather*} P_{1.6} = I V_{1.6} = (3.18 \,\text{A}) (5.09 \,\text{V}) = \boxed{16.18 \,\text{W}}\\ P_{2.4} = IV_{2.4} = (3.18 \,\text{A}) (7.63 \,\text{V}) = \boxed{24.27 \,\text{W}}\\ P_{4.8} = IV_{4.8} = (3.18 \,\text{A}) (15.26 \,\text{V}) = \boxed{48.54 \,\text{W}} \end{gather*} (f) As in part (e), the most dissipated power is due to the $\textbf{greatest resistance}$
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