Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 21 - Electric Current and Direct-Current Circuits - Problems and Conceptual Exercises - Page 761: 120

Answer

Please see the work below.

Work Step by Step

Given that the resistors are connected in parallel, $ power \space dissipated \space in \space R_1\space P_1=\frac{V^2}{R_1}$ $ power \space dissipated \space in \space R_2\space P_2=\frac{V^2}{R_2}$ Thus, the net power is $ P_1+P_2=\frac{V^2}{R_1}+\frac{V^2}{R_2}=V^2(\frac{R_2+R_1}{R_1R_2})$ Now, the equivalent resistance of the circuit when the resistors are connected in parallel is given as $ R_{eq}=(\frac{1}{R_1}+\frac{1}{R_2})^{-1}$ $ R_{eq}=(\frac{R_1+R_2}{R_1R_2})^{-1}$ Thus, the net power is $ P_{total}=V^2(\frac{R_1+R_2}{R_1R_2})$ Thus, in both cases the net power is the same.
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