Thomas' Calculus 13th Edition

Published by Pearson
ISBN 10: 0-32187-896-5
ISBN 13: 978-0-32187-896-0

Chapter 9: First-Order Differential Equations - Section 9.2 - First-Order Linear Equations - Exercises 9.2 - Page 537: 25

Answer

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

Work Step by Step

Consider $\dfrac{di}{dt}+(\dfrac{R}{T}) i=\dfrac{V}{L}$ Recall the formula: $i=(\dfrac{V}{R})(1-e^{-(\frac{R}{L})t})$ When the value of steady current becomes: $i=(\dfrac{1}{2})(\dfrac{V}{R})$, then we get $(\dfrac{1}{2})(\dfrac{V}{R})=(\dfrac{V}{R})(1-e^{-(\frac{R}{L})t})$ This implies that $\ln (1)-\ln (2)=\ln e^{-(\frac{R}{L})t}$ or, $-\ln (2)=\ln e^{-(\frac{R}{L})t}$ Hence, $t=\dfrac{L}{R} \ln (2)$ seconds
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