A dipole having dipole moment p is in front of a solid uncharged conducting sphere as shown in the figure. The net potential at point A lying on the surface of the sphere is: (where, K=14πε0)
A
Kpcosϕr2
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B
Kpcos2ϕr2
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C
zero
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D
2Kpcos2ϕr2
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Solution
The correct option is BKpcos2ϕr2 Electric potential due to an electric dipole: V=K→p.→rr3
Potential at the centre of sphere V=K→p(rcosϕ)(rcosϕ)3=Kpcos2ϕr2
∵ This is conducting sphere, so potential at all points of sphere is same.