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 762: 128

Answer

a) $ V_1: 12.0V $ $ V_2: 4.8V $ $ V_3: 7.2V $ b) $ R_1: 0.12A $ $ R_2: 0.02A $ $ R_3: 0.02A $

Work Step by Step

(a) We know that $ R_1$ is connected across the battery; the potential difference across it will be same as the emf, which is $12.0V $. The resistances $ R_2$ and $ R_3$ are in series and their combined potential difference will be the emf. Since $ R_3$ is $\frac{3}{2}$ times $ R_2$, the potential difference across $ R_3$ will also be $\frac{3}{2}$ times the potential difference across $ R_2$. Let $ x $ be the potential difference across $ R_2$: $ x+\frac{3}{2}x=12$ $\implies x=4.8V $ Now the potential difference across $ R_3$ will be $12-4.8=7.2V $. Thus, the potential difference across each resistor is as follows: $ V_1: 12.0V $ $ V_2:4.8V $ $ V_3:7.2V $ (b) We can find the required currents as follows: $ I_1=\frac{V_1}{R_1}$ $ I_1=\frac{12.0V}{100\Omega}$ $ I_1=0.12A $ The current through $ R_2$ is $ I_2=\frac{V_2}{R_2}$ We plug in the known values to obtain: $ I_2=\frac{4.8V}{200\Omega}$ $ I_2=0.02A $ As $ R_2$ and $ R_3$ are in series, hence the current though them will be the same. Thus, the current through each resistor is as follows: $ R_1: 0.12A $ $ R_2: 0.02A $ $ R_3: 0.02A $
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