
For inside part
J=πR2I
∫B⋅dl=μ0Iinclosed…(i)
B2πr=μ0(πR2I)×πr2
B2πr=μ0IR2r2
B∝r
For outside part
∫B⋅dl=μ0Iinclosed
B(2πr)=μ0I
∴B∝r1

NEET UG 2021 — Physics Electromagnetism
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:
Held on 30 Apr 2021 · Verified 9 Jul 2026.




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