Q.
The electric potential due to an extremely short dipole at a distance r from it is proportional to
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Electrostatic Potential and Capacitance
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Solution:
Potential at point P=r1KV−r2KV V=KV(r1r2r2−r1)
we are taking extremely short dipole r1≅r2=r r2−r1≅dcosθ V=r2KVdcos theta V=r2KPcos theta P=Vd,
where P is the dipole moment. ∴V∝r21