Electrostatic potential due to charge configuration at a far point P is
A
kqdr2
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B
zero
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C
kqd2r2
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D
√3kqd2r2
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Solution
The correct option is Ckqd2r2 Since point P is far it can be treated as point dipole. Therefore, V=K→p.→rr3=kpcosθr2=kqd2r2 As, →p.⇀r=prcosθ where, cos60°=12 and p=qd.