Q.

For a short dipole placed at origin O, the dipole moment P is along x-axis, as shown in the figure. If the electric potential and electric field at A are V0 and E0, respectively, then the correct combination of the electric potential and electric field, respectively, at point B on the y-axis is given by
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a

V0andE04

b

V02andE016

c

zero andE016

d

zero andE08

answer is C.

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Detailed Solution

Understanding the Problem

We have a short dipole placed at the origin OO with its dipole moment PP along the x-axis.

  • Point A is on the axial line at a distance rr from the dipole.
  • Point B is on the equatorial line at a distance 2r2r from the dipole.

Given:

  • The electric potential at AA is V0V_0.
  • The electric field at AA is E0E_0.

We need to determine the electric potential and electric field at point B.

Step 1: Electric Potential of a Dipole

The electric potential VV due to a short dipole at a point at distance rr is:

V=14πϵ0pr^r2V = \frac{1}{4\pi\epsilon_0} \cdot \frac{\mathbf{p} \cdot \hat{r}}{r^2}

On the axial line (Point A at distance rr):

  • VA=14πϵ0pr2=V0V_A = \frac{1}{4\pi\epsilon_0} \cdot \frac{p}{r^2} = V_0

On the equatorial line (Point B at distance 2r2r):

Since the dipole potential is given by:

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

and on the equatorial line θ=90cos90=0\theta = 90^\circ \Rightarrow \cos90^\circ = 0,

  • VB=0V_B = 0

Thus, the electric potential at B is zero.

 

Step 2: Electric Field of a Dipole

The magnitude of the electric field at a distance rr from a dipole:

On the axial line:

Eaxial=14πϵ02pr3E_{\text{axial}} = \frac{1}{4\pi\epsilon_0} \cdot \frac{2p}{r^3}

Given that at AA (on the axial line at rr), the field is E0E_0:

EA=E0=14πϵ02pr3E_A = E_0 = \frac{1}{4\pi\epsilon_0} \cdot \frac{2p}{r^3}

On the equatorial line:

Eequatorial=14πϵ0pr3E_{\text{equatorial}} = \frac{1}{4\pi\epsilon_0} \cdot \frac{p}{r^3}

At B (distance 2r2r):

EB=14πϵ0p(2r)3=14πϵ0p8r3E_B = \frac{1}{4\pi\epsilon_0} \cdot \frac{p}{(2r)^3} = \frac{1}{4\pi\epsilon_0} \cdot \frac{p}{8r^3}

Since E0=14πϵ02pr3E_0 = \frac{1}{4\pi\epsilon_0} \cdot \frac{2p}{r^3}, we can express EBE_B in terms of E0E_0:

EB=E016E_B = \frac{E_0}{16}

Final Answer:

  • Electric potential at B00
  • Electric field at BE016\frac{E_0}{16}
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For a short dipole placed at origin O, the dipole moment P is along x-axis, as shown in the figure. If the electric potential and electric field at A are V0 and E0, respectively, then the correct combination of the electric potential and electric field, respectively, at point B on the y-axis is given by