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Magnetics question

2022 · 28 Jun · Shift 1 · Q52
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  5. /2022 · 28 Jun · Shift 1 · Q52

Magnetics question

2022 · 28 Jun · Shift 1 · Q52

JEE MainPhysicsMagneticsMCQ+4 / −1
An infinitely long hollow conducting cylinder with radius R carries a uniform current along its surface. Choose the correct representation of magnetic field (B) as a function of radial distance (r) from the axis of cylinder.
  1. A
    JEE Main 2022 (Online) 28th June Morning Shift Physics - Magnetic Effect of Current Question 107 English Option 1
  2. B
    JEE Main 2022 (Online) 28th June Morning Shift Physics - Magnetic Effect of Current Question 107 English Option 2
  3. C
    JEE Main 2022 (Online) 28th June Morning Shift Physics - Magnetic Effect of Current Question 107 English Option 3
  4. D
    JEE Main 2022 (Online) 28th June Morning Shift Physics - Magnetic Effect of Current Question 107 English Option 4
View written solutionFree

Correct answer: D

  1. Understand the current distribution

An infinitely long hollow conducting cylinder of radius RRR carries current uniformly along its surface and parallel to its axis.

So the current is confined only at r=Rr=Rr=R.


  1. Use Ampere's circuital law

For a long cylindrical current distribution, by symmetry the magnetic field is tangential and depends only on radial distance rrr.

Thus,

∮B⃗⋅dl⃗=B(2πr)=μ0Ienc\oint \vec B \cdot d\vec l = B(2\pi r)=\mu_0 I_{\text{enc}}∮B⋅dl=B(2πr)=μ0​Ienc​

Now consider two regions.


  1. Region 1: Inside the hollow cylinder (r<Rr<Rr<R)

Since all the current lies on the surface at r=Rr=Rr=R, an Amperian loop of radius r<Rr<Rr<R encloses no current:

Ienc=0I_{\text{enc}}=0Ienc​=0

Hence,

B(2πr)=0  ⟹  B=0B(2\pi r)=0 \implies B=0B(2πr)=0⟹B=0

So,

B=0for r<RB=0 \quad \text{for } r<RB=0for r<R
  1. Region 2: Outside the cylinder (r>Rr>Rr>R)

Now the Amperian loop encloses the full current III:

Ienc=II_{\text{enc}}=IIenc​=I

Therefore,

B(2πr)=μ0IB(2\pi r)=\mu_0 IB(2πr)=μ0​I B=μ0I2πrB=\frac{\mu_0 I}{2\pi r}B=2πrμ0​I​

So,

B=μ0I2πrfor r>RB=\frac{\mu_0 I}{2\pi r} \quad \text{for } r>RB=2πrμ0​I​for r>R
  1. Behavior at r=Rr=Rr=R

Just inside the surface:

Binside=0B_{\text{inside}}=0Binside​=0

Just outside the surface:

Boutside=μ0I2πRB_{\text{outside}}=\frac{\mu_0 I}{2\pi R}Boutside​=2πRμ0​I​

So the graph has:

  • B=0B=0B=0 for all r<Rr<Rr<R
  • a sudden jump at r=Rr=Rr=R
  • then decreases as 1/r1/r1/r for r>Rr>Rr>R

  1. Match with the correct graph

The correct representation must show:

  • zero field inside,
  • discontinuity at r=Rr=Rr=R,
  • inverse radial decay outside.

That corresponds to Option D.


  1. Comparison with stored answer

Stored correct answer = D.

My derived answer = D.

So they agree.

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