Fundamentals of Physics Extended (10th Edition)

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

Chapter 21 - Coulomb's Law - Problems - Page 628: 50a

Answer

x = $\frac{L}{2}$(1 + $\frac{kQq}{Wh^2}$) {where, k = $\frac{1}{4\pi\epsilon_0}$}

Work Step by Step

The rod is balanced. Hence, net torque ($\tau$) = 0 So, $\tau$ (clockwise) = $\tau$ (anti-clockwise) Here, F1 and W are applying torque in a clockwise direction, whereas, F2 is applying torque in an anti-clockwise direction...... (1) We know that, $\tau$ = rFsin$\theta$...... (2) where r = distance from pivot point. Torque caused by F1 = ($\frac{kQq}{h^2}$)($\frac{L}{2}$) = $\frac{kQqL}{2h^2}$ clockwise ......(3) Torque caused by F2 = ($\frac{2kQq}{h^2}$)($\frac{L}{2}$) = $\frac{kQqL}{h^2}$ anti-clockwise ......(4) Torque caused by W = W(x-$\frac{L}{2}$) = $\frac{W}{2}$(2x-L) clockwise ......(5) Using (1), (3), (4) and (5): $\frac{kQqL}{2h^2}$ + $\frac{W}{2}$(2x-L) = $\frac{kQqL}{h^2}$ $\frac{W}{2}$(2x-L) = $\frac{kQqL}{2h^2}$ 2x-L = $\frac{kQqL}{Wh^2}$ 2x = L + $\frac{kQqL}{Wh^2}$ Thus, x = $\frac{L}{2}$(1 + $\frac{kQq}{Wh^2}$) {where, k = $\frac{1}{4\pi\epsilon_0}$}
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