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Question: The centres of two thin coaxial conducting loops of radius $r$ each are separated by distance $d(d >...

The centres of two thin coaxial conducting loops of radius rr each are separated by distance d(d>>r)d(d >> r). Then, the mutual inductance of the system is (coil lies in vertical plane such that both coils plane facing each other)

A

μ0πr22d\frac{\mu_0 \pi r^2}{2d}

B

μ0πr22d3\frac{\mu_0 \pi r^2}{2d^3}

C

μ0πr42d3\frac{\mu_0 \pi r^4}{2d^3}

D

μ0πr42d\frac{\mu_0 \pi r^4}{2d}

Answer

μ0πr42d3\frac{\mu_0 \pi r^4}{2d^3}

Explanation

Solution

To find the mutual inductance of two thin coaxial conducting loops of radius rr each, separated by a distance dd where drd \gg r:

  1. Assume a current in one loop: Let a current II flow through the first loop (Loop 1).

  2. Calculate the magnetic field produced by Loop 1 at the location of Loop 2: The magnetic field on the axis of a circular loop of radius rr carrying current II at a distance zz from its center is given by: Bz=μ0Ir22(r2+z2)3/2B_z = \frac{\mu_0 I r^2}{2(r^2 + z^2)^{3/2}} Since the two loops are separated by a distance dd and drd \gg r, we can approximate the magnetic field at the center of Loop 2 (i.e., at z=dz=d) by neglecting r2r^2 in the denominator compared to d2d^2: B1μ0Ir22(d2)3/2=μ0Ir22d3B_1 \approx \frac{\mu_0 I r^2}{2(d^2)^{3/2}} = \frac{\mu_0 I r^2}{2d^3}

  3. Calculate the magnetic flux through Loop 2 due to the current in Loop 1: Since drd \gg r, the magnetic field produced by Loop 1 can be considered approximately uniform over the small area of Loop 2, and its direction is along the axis. The area of Loop 2 is A2=πr2A_2 = \pi r^2. The magnetic flux Φ21\Phi_{21} through Loop 2 due to the current II in Loop 1 is: Φ21=B1×A2\Phi_{21} = B_1 \times A_2 Φ21=(μ0Ir22d3)(πr2)\Phi_{21} = \left(\frac{\mu_0 I r^2}{2d^3}\right) (\pi r^2) Φ21=μ0πIr42d3\Phi_{21} = \frac{\mu_0 \pi I r^4}{2d^3}

  4. Determine the mutual inductance: The mutual inductance MM is defined as the ratio of the magnetic flux through one loop to the current in the other loop: M=Φ21IM = \frac{\Phi_{21}}{I} Substituting the expression for Φ21\Phi_{21}: M=μ0πIr42d3IM = \frac{\frac{\mu_0 \pi I r^4}{2d^3}}{I} M=μ0πr42d3M = \frac{\mu_0 \pi r^4}{2d^3}

The mutual inductance of the system is μ0πr42d3\frac{\mu_0 \pi r^4}{2d^3}.