Q.

A thick current carrying cable of radius R carries current I uniformly distributed across its cross-section. The variation of magnetic field B(r) due to the cable with the distance r from the axis of the cable is represented by          [2021]

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Ans.

(4)

By Ampere's circuital law,

B·dl=μ0×current losed by path

B·2πr=μ0×Ir2a2  (R=a)

B=μ0Ir2πa2  (for r<a)

At surface r=a, so B=μ0I2πa

    B=μ0I2πr  (for r>a)

The variation of magnetic field with distance 'r' from the axis is given by the above figure.