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A thin circular wire of radius r has a charge Q. If a point charge q is placed at the centre of the ring, then find the increase in tension in the wire.

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Consider an element. Its enlarged view is as shown. For equilibrium of this segment, we can write.
`F= 2DeltaT sin ((d theta)/(2))`
Here F is the repulsive force between q and elemental charge dQ
`dQ=(Q)/( 2pi R) (Rd theta)`
The electric outward force on element is
`F=(1)/(4pi in_(0)) (qdQ)/( R^(2))`
From the above three equations, we can write
`(1)/(4pi in_(0)) (q)/(R^(2)) (QRd theta)/(2piR) ~~ 2DeltaT((d theta)/(2))`
(`:. sin alpha = alpha` for small angle)
`Delta = (Qq)/( 8pi^(2) in_(0) R^(2))`
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