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NEET PHYSICSMedium

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:

A

Graph showing B linearly increasing for r < R and decreasing as 1/r for r > R

B

Graph showing B constant for r < R and decreasing for r > R

C

Graph showing B zero for r < R and decreasing for r > R

D

Graph showing B increasing parabolically for r < R and decreasing for r > R

Step-by-Step Solution

  1. Region 1: Inside the cable (r<Rr < R): Apply Ampere's Circuital Law: Bdl=μ0Ienclosed\oint \mathbf{B} \cdot d\mathbf{l} = \mu_0 I_{enclosed}. For a path of radius rr inside the wire, the current enclosed is a fraction of the total current II, proportional to the area: Ienclosed=I(πr2πR2)=Ir2R2I_{enclosed} = I \left(\frac{\pi r^2}{\pi R^2}\right) = I \frac{r^2}{R^2} B(2πr)=μ0Ir2R2B(2\pi r) = \mu_0 I \frac{r^2}{R^2} B=(μ0I2πR2)rB = \left(\frac{\mu_0 I}{2\pi R^2}\right) r Thus, BrB \propto r (Linear increase passing through the origin).
  2. Region 2: Outside the cable (rRr \geq R): The enclosed current is the total current II. B(2πr)=μ0IB(2\pi r) = \mu_0 I B=μ0I2πrB = \frac{\mu_0 I}{2\pi r} Thus, B1rB \propto \frac{1}{r} (Rectangular hyperbola decrease).
  3. Conclusion: The magnetic field increases linearly from zero at the axis to a maximum at the surface (r=Rr=R), and then decreases inversely with distance outside. This corresponds to the standard graph for a solid cylindrical wire .
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