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NEET PHYSICSMedium

From Ampere's circuital law, for a long straight wire of circular cross-section carrying a steady current, the variation of the magnetic field inside and outside the region of the wire is:

A

A linearly decreasing function of distance upto the boundary of the wire and then a linearly increasing one for the outside region.

B

Uniform and remains constant for both regions.

C

A linearly increasing function of distance upto the boundary of the wire and then a linearly decreasing one for the outside region.

D

A linearly increasing function of distance r upto the boundary of the wire and then decreasing one with 1/r dependence for the outside region.

Step-by-Step Solution

  1. Inside the Wire (r<ar < a): Assuming the current II is uniformly distributed over the cross-section of radius aa, the current enclosed by a loop of radius rr is Ienclosed=I(r2/a2)I_{enclosed} = I(r^2/a^2). Applying Ampere's Law: B(2πr)=μ0I(r2/a2)    B=(μ0I2πa2)rB(2\pi r) = \mu_0 I(r^2/a^2) \implies B = \left(\frac{\mu_0 I}{2\pi a^2}\right)r. Thus, the magnetic field is directly proportional to the distance (BrB \propto r), representing a linear increase.
  2. Outside the Wire (r>ar > a): The current enclosed is the total current II. Applying Ampere's Law: B(2πr)=μ0I    B=μ0I2πrB(2\pi r) = \mu_0 I \implies B = \frac{\mu_0 I}{2\pi r}. Thus, the magnetic field is inversely proportional to the distance (B1/rB \propto 1/r).
  3. Conclusion: The field increases linearly up to the boundary and then decreases with 1/r1/r dependence outside.
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