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Electric field due to an electric dipole at a point on its axial line: AB is an electric dipole of two point charges −q and +q separated by small distance 2d. P is a point along the axial line of the dipole at a distance r from the midpoint O of the electric dipole.
The electric fiedl at the point P due to +q placed at B is,
(along BP)
The electric field at the point P due to −q placed at A is,
Therefore, the magnitude of resultant electric field (E) acts in the direction of the vector with a greater, magnitude. The resultant electric field at P is
E= E1 +(−E2)
along BP
along BP
along BP
along BP
[∵ Electric dipole moment p=q×2d]
E acts in the direction of dipole moment.
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