JEE Challenger
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Work Done Bringing Dipole Near Current Loop

The work required to bring the magnetic dipole from infinity to a distance rr from the center of the loop during the specified process is proportional to:

Options

A

m/r5m/r^5

B

m2/r5m^2/r^5

C

m2/r6m^2/r^6

Correct
D

m2/r7m^2/r^7

Step-by-Step Solution

To find the work required to bring the magnetic dipole from infinity to a distance rr from the center of the loop, we analyze the interaction between the dipole and the induced current in the loop.

1. Magnetic Flux through the Loop

Consider a circular loop of radius aa and a small magnetic dipole of magnetic moment mm located on its axis at a distance rr (r≫ar \gg a) from its center.

The magnetic field generated along the axis by a loop carrying a unit current I=1I = 1 at distance rr is: B(r)=μ0a22(a2+r2)3/2≈μ0a22r3B(r) = \frac{\mu_0 a^2}{2(a^2 + r^2)^{3/2}} \approx \frac{\mu_0 a^2}{2 r^3}

Using the reciprocity property of mutual inductance, the magnetic flux Φ\Phi passing through the loop due to the dipole mm located at distance rr is: Φ=B(r)⋅m=μ0a2m2r3\Phi = B(r) \cdot m = \frac{\mu_0 a^2 m}{2 r^3}

2. Induced Current in the Loop

During the process of bringing the dipole from infinity to position rr, the change in magnetic flux induces a current II in the loop. By flux conservation (or self-inductance relation LI+Φ=0L I + \Phi = 0): I=−ΦL=−μ0a2m2Lr3I = -\frac{\Phi}{L} = -\frac{\mu_0 a^2 m}{2 L r^3}

3. Magnetic Force on the Dipole

The magnetic force acting on the dipole along the axis of the loop is given by: Fmag=I∂Φ∂rF_{\text{mag}} = I \frac{\partial \Phi}{\partial r}

Substituting II and ∂Φ∂r\frac{\partial \Phi}{\partial r}: ∂Φ∂r=∂∂r(μ0a2m2r3)=−3μ0a2m2r4\frac{\partial \Phi}{\partial r} = \frac{\partial}{\partial r}\left(\frac{\mu_0 a^2 m}{2 r^3}\right) = -\frac{3 \mu_0 a^2 m}{2 r^4}

Fmag=(−μ0a2m2Lr3)(−3μ0a2m2r4)=3μ02a4m24Lr7F_{\text{mag}} = \left(-\frac{\mu_0 a^2 m}{2 L r^3}\right) \left(-\frac{3 \mu_0 a^2 m}{2 r^4}\right) = \frac{3 \mu_0^2 a^4 m^2}{4 L r^7}

4. Work Done by External Agent

The work required by an external agent to bring the dipole quasi-statically from infinity to distance rr against the magnetic force is: W=∫∞r−Fmag dr′W = \int_{\infty}^r -F_{\text{mag}} \, dr'

W=−∫∞r3μ02a4m24Lr′7 dr′=[μ02a4m28Lr′6]∞r=μ02a4m28Lr6W = -\int_{\infty}^r \frac{3 \mu_0^2 a^4 m^2}{4 L r'^7} \, dr' = \left[ \frac{\mu_0^2 a^4 m^2}{8 L r'^6} \right]_{\infty}^r = \frac{\mu_0^2 a^4 m^2}{8 L r^6}

Thus, the work done WW is proportional to: W∝m2r6W \propto \frac{m^2}{r^6}

Correct Option: (C)