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Q. Two equal negative charges $-q$ are fixed at points $(0, a)$ and $(0,-a)$ on the $y$ -axis. A positive charge $Q$ is released from rest at the point $(2 a, 0)$ on the $x$ -axis. The charge $Q$ will

Electric Charges and Fields

Solution:

By symmetry of problem, the components of force on $Q$ due to charges at $A$ and $B$ along $y$ -axis will cancel each other while along $x$ -axis will add up and will be along $C O .$ Under the action of this force, charge $Q$ will move towards $O$. If at any time charge $Q$ is at a distance $x$ from $O$
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$F=2 \frac{1}{4 \pi \varepsilon_{0}} \frac{-q Q}{\left(a^{2}+x^{2}\right)} \times \frac{x}{\left(a^{2}+x^{2}\right)^{1 / 2}}$
i.e., $\quad F=-\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{2 q Q x}{\left(a^{2}+x^{2}\right)^{3 / 2}}$
As the restoring force $F$ is not linear, motion will be oscillatory (with amplitude $2 a$ ) but not simple harmonic.