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 625: 10a

Answer

$\frac{Q}{q} = -2\sqrt 2$

Work Step by Step

$F_{on. 1} = F_{2 on 1} + F_{3on1} + F_{4on1}$ Since $q_1 = q_2$ the charges have the same sign and repel each other The formula for the electrostatic force of $q_4$ on $q_1$: $ F_{4on1} = \frac{Kq_1q_2}{r^2_{14}}$ ${r^2_{14}} = a^2 +a^2 = 2a^2$ $ F_{4on1,x} = \frac{Kq_1q_2}{r^2_{14}}(-cos(45))$ $ F_{4on1,y} = \frac{Kq_1q_2}{r^2_{14}}(sin(45))$ $ F_{4on1} = \frac{Kq_1q_2}{r^2_{14}}(-cos(45) +sin(45))$ $ F_{4on1} = \frac{KQ^2}{2a^2}(-\frac{1}{\sqrt 2} i+\frac{1}{\sqrt 2} j)$ $ F_{4on1} = \frac{KQ^2}{2\sqrt 2 a^2}(- i+j)$ In order for $F_{2on1}$ must be in the +$i$ direction to cancel the x component on $F_{4on1}$ and $F_{3on1}$ must be in the -$ j $ This means that charges Q and q must have opposite signs $ F_{2on1} = \frac{Kq_1q_2}{r^2_{12}}$ $r^2_{12} = a^2$ $ F_{2on1} = \frac{Kq_1q_2}{a^2}$ $ F_{2on1} = \frac{kQq}{a^2}(-i)$ $ F_{3on1} = \frac{KQq}{a^2}(-j)$ For the net to be zero the x components must be added together to equal zero: $ F_{2on1} + F_{4on1,x} = \frac{KQq}{a^2}(-i) + \frac{KQ^2}{r^2_{14}}(-cos(45)) = 0$ $\frac{KQ}{a^2}(q-\frac{Q}{2\sqrt 2 }) = 0$ $q-\frac{Q}{2\sqrt 2 } = 0$ $\frac{|Q|}{|q|}= 2\sqrt 2$ Since Q and q have opposite signs the answer must be negative: $\frac{|Q|}{|q|}= -2\sqrt 2$
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