derive an expression for the elecric field at a point on the eauatorial position of an electric dipole
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Consider an electric dipole consisting of two point changes −q and +q separated by a small distance AB=2a with center O and dipole moment P=q(2a)
Let OP=r
E1= electric intensity at P due to change -q at A.
∴|E1−→|=14π∈0qAP2
AP2=OP2+OA2
=r2+a2
∴|E1−→|=14π∈0qr2+a2
E1−→=Pc−→
Let ∠PBA=∠PAB=θ.
E1 has two components E1 can θ along PR∥BA and E1sinθ along PE⊥BA .
If E2 is the electric intensity at P, due to change +q at B, then
E2−→=14π∈0qBp2=14π∈0q(r2+a2)
E2−→ is along PD−→−
This has two components, E2 is along PR∥BA and E2sinθ along PF.
E→=2E1cosθ
=24π∈0.q(r2+q2)cosθ
=24π∈0.q(r2+a2)(OAAD)
=24π∈0.q(r2+q2)ar2+a2−−−−−√
=q×2a4π∈0(r2+a2)3/2
But q×2a=|P→|, the dipole moment
∴|E→|=|P→|4π∈0(r2+a2)3/2
The direction of E→ is along .
PR−→−||BA−→− (ie) opposite to P→
or E→=−P→4π∈0(r2+a2)3/2
If the dipole is short 2a<<r
|E→|=|P→|4π∈0r3
|E→|α1r3..
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