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➝ The amount of work done against the electrostatic force to move a unit positive charge from one point to another is known a potential due to electric dipole.
Derivation :-
Potential at +q {V(+q)} =
Potential at -q {V(-q)} =
Vp = V+q + V-q ( Total V )
➝ V = +
➝ V =
➝ V =
➝ V =
➝ V =
➝ V =
We know that,
| p = 2aq |
So,
➝ V =
r² - a² ≈ r²
Where, short dipole
Where, short dipole a² ➝ 0 , w.r.t r , [ r >> a ]
Hence, V = ![\dfrac{1}{4\pi \:Eo } \dfrac{p}{ {r}^{2} } \dfrac{1}{4\pi \:Eo } \dfrac{p}{ {r}^{2} }](https://tex.z-dn.net/?f=+%5Cdfrac%7B1%7D%7B4%5Cpi+%5C%3AEo+%7D++%5Cdfrac%7Bp%7D%7B+%7Br%7D%5E%7B2%7D+%7D+)
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may this answer helps you ....=_=
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