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 760: 98

Answer

$0.99W; 1.32W; 1.13W$

Work Step by Step

We know that at the junction $I=I_1+I_2$....eq(1) In the lower closed loop $12V-I(12\Omega)-I_1(65\Omega)=0$ This simplifies to: $I_1=\frac{12}{65}-\frac{12}{65}I$.....eq(2) In the upper closed loop $12V-I(12\Omega)-I_2(55\Omega)=0$ This simplifies to: $I_2=\frac{12}{55}-\frac{12}{55}I$....eq(3) We plug in values from eq(2) and eq(3) in eq(1) to obtain: $I=(\frac{12}{65})-(\frac{12}{65})I+(\frac{12}{65})-(\frac{12}{65})I$ This simplifies to: $I=0.287A$ We plug in this value in eq(2) to obtain: $I_1=\frac{12}{65}-\frac{12}{65}(0.287A)$ $\implies I_1=0.132A$ and from eq(1) $I_2=I-I_1$ $I_2=0.287A-0.132A$ $I_2=0.155A$ Now the power dissipated in the $12\Omega$ resistor $P_{12}=(0.287A)^2(12\Omega)=0.99W$ Power dissipated in $55\Omega$ $P_{55}=(0.155A)^2(55\Omega)=1.32W$ Power dissipated in $65\Omega$ $P_{65}=(0.132A)^2(65\Omega)=1.13W$
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