With the help of a labelled diagram, obtain an expression for the electric field intensity ‘E’ at a point P in broad side position (i.e., equatorial plane) of an electric dipole.  - Zigya
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With the help of a labelled diagram, obtain an expression for the electric field intensity ‘E’ at a point P in broad side position (i.e., equatorial plane) of an electric dipole. 


Electric field intensity at a point on the broad side-on position equatorial line: Consider an electric dipole consisting of two equal but opposite charges -q and +q separated by a vector distance 2l. Let P be a point at a distance r from the centre of the dipole O. The electric intensity at P due to the dipole is the vector sum of the field due to the charge -q at A and +q at B.


Electric intensity at P due to - q = EA

But    AP2 = r2 +l2;    

where AO = OB = l

Magnitude of EA is |EA| = 







The resultant intensity is the vector sum of.

EA and EB can be resolved into two components.

The y-components of the fields cancel each other because E
A sin θ = EB sin θ and they are oppositely directed. The x-components add up to give the resultant field E.



From the above two equations for Eeq and Eaxial we find that the electric intensity at an axial point is twice the electric intensity at a point on the equatorial position, lying at the same distance from the centre of the dipole.
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