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Question: A small magnet is placed on the axis, at a distance $\frac{3a}{4}$ from center of a fixed conducting...

A small magnet is placed on the axis, at a distance 3a4\frac{3a}{4} from center of a fixed conducting ring of radius aa and resistance RR. When it is moved from that point to infinity, charge qq flows through the ring then magnetic moment of magnet is

A

27aRq32μ0\frac{27aRq}{32\mu_0}

B

32aRq27μ0\frac{32aRq}{27\mu_0}

C

27μ0a32Rq\frac{27\mu_0a}{32Rq}

D

32μ0a27Rq\frac{32\mu_0a}{27Rq}

Answer

27aRq32μ0\frac{27aRq}{32\mu_0}

Explanation

Solution

The total charge qq flowing through the ring is given by q=ΔΦBRq = \frac{\Delta \Phi_B}{R}. The magnetic flux through the ring due to a magnetic dipole on its axis at distance dd is ΦB=μ0ma22d3\Phi_B = \frac{\mu_0 m a^2}{2 d^3}. Initial flux at d1=3a4d_1 = \frac{3a}{4} is ΦB1=μ0ma22(3a4)3=32μ0m27a\Phi_{B1} = \frac{\mu_0 m a^2}{2 (\frac{3a}{4})^3} = \frac{32 \mu_0 m}{27a}. Final flux at d2=d_2 = \infty is ΦB2=0\Phi_{B2} = 0. So, ΔΦB=ΦB2ΦB1=32μ0m27a\Delta \Phi_B = \Phi_{B2} - \Phi_{B1} = -\frac{32 \mu_0 m}{27a}. Therefore, q=ΔΦBR=32μ0m27aRq = \frac{|\Delta \Phi_B|}{R} = \frac{32 \mu_0 m}{27aR}. Solving for mm, we get m=27aRq32μ0m = \frac{27aRq}{32\mu_0}.