Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 27 - Circuits - Problems - Page 799: 57

Answer

$t = 2.08\times 10^{-4}~s$

Work Step by Step

The potential across the capacitor will be equal to the potential across the resistor when the potential across the capacitor is half of the battery emf. We can find the time $t$: $\frac{q}{C} = \mathscr{E}~(1-e^{-t/\tau}) = 0.500~\mathscr{E}$ $1-e^{-t/\tau} = 0.500$ $e^{-t/\tau} = 0.500$ $e^{t/\tau} = 2.00$ $\frac{t}{\tau} = ln(2.00)$ $t = ln(2.00)~\tau$ $t = ln(2.00)RC$ $t = [ln(2.00)]~(20.0~\Omega)~(15.0~\mu F)$ $t = 2.08\times 10^{-4}~s$
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