University Calculus: Early Transcendentals (3rd Edition)

Published by Pearson
ISBN 10: 0321999584
ISBN 13: 978-0-32199-958-0

Chapter 16 - Section 16.2 - First-Order Linear Equations - Exercises - Page 16-14: 25

Answer

$t=\dfrac{L}{R} \ln (2)$ seconds

Work Step by Step

Here, we have $\dfrac{di}{dt}+\dfrac{R}{T}i=\dfrac{V}{L}$ As we know that $i=\dfrac{V}{R}(1-e^{-(\frac{R}{L})t})$ The value of steady current becomes: $i=(\dfrac{1}{2})(\dfrac{V}{R})$ Then, we have $(\dfrac{1}{2})(\dfrac{V}{R})=\dfrac{V}{R}(1-e^{-(\frac{R}{L})t})$ $\implies \ln (1)-\ln (2)=\ln e^{-(\frac{R}{L})t}$ Thus, we get $t=\dfrac{L}{R} \ln (2)$ seconds
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