The electric field due to a dipole on the axial line.
- you can see that, if the point P is far away i.e., r>>l, then
we can reduce the expression to (2.K.q.l)/r3
where q.l is defined as the electric dipole moment of the dipole of length l
If P is outside the dipole,
→E at P due to +q=kq(r−l2)2(^x)
→E at P due to −q=+kq(r+l2)2(−^x)
Total electric field at P,E=kq[1(r−l2)2−l(r+l2)2]
E=2kqlr(r2−l24)2(^x)