Solveeit Logo

Question

Question: Consider a point A far away from short dipole p. By keeping r constant, $\theta$ varies from 0° to 3...

Consider a point A far away from short dipole p. By keeping r constant, θ\theta varies from 0° to 360°. Variation of potential of dipole at A with respect to θ\theta:-

A

Graph (1)

B

Graph (2)

C

Graph (3)

D

Graph (4)

Answer

Graph (1) correctly represents the variation of potential of a dipole with respect to θ\theta.

Explanation

Solution

The electric potential VV at a point (r,θ)(r, \theta) due to a short electric dipole of dipole moment p\vec{p} is given by the formula:

V=14πϵ0pcosθr2V = \frac{1}{4\pi\epsilon_0} \frac{p \cos\theta}{r^2}

In this problem, the point A is far away from the dipole, so the short dipole approximation is valid. We are given that rr is constant, and θ\theta varies from 0° to 360°.

Since pp, rr, and 14πϵ0\frac{1}{4\pi\epsilon_0} are constants, the potential VV is directly proportional to cosθ\cos\theta.

VcosθV \propto \cos\theta

Let's analyze the behavior of cosθ\cos\theta as θ\theta varies from 0° to 360°:

  • At θ=0\theta = 0^\circ: cos(0)=1\cos(0^\circ) = 1. So, VV will be maximum positive.
  • At θ=90\theta = 90^\circ: cos(90)=0\cos(90^\circ) = 0. So, VV will be zero.
  • At θ=180\theta = 180^\circ: cos(180)=1\cos(180^\circ) = -1. So, VV will be maximum negative.
  • At θ=270\theta = 270^\circ: cos(270)=0\cos(270^\circ) = 0. So, VV will be zero.
  • At θ=360\theta = 360^\circ: cos(360)=1\cos(360^\circ) = 1. So, VV will be maximum positive (same as at 0°).

Therefore, Graph (1) correctly represents the variation of potential of a dipole with respect to θ\theta.