MCQMediumJEE 2025Ampere's Law

JEE Physics 2025 Question with Solution

Consider a long straight wire of a circular cross-section (radius aa) carrying a steady current II. The current is uniformly distributed across this cross-section. The distances from the centre of the wire's cross-section at which the magnetic field (inside the wire, outside the wire) is half of the maximum possible magnetic field, anywhere due to the wire, will be:

  • A

    [a2,3a]\left[ \frac{a}{2}, 3a \right]

  • B

    [a2,2a]\left[ \frac{a}{2}, 2a \right]

  • C

    [a4,2a]\left[ \frac{a}{4}, 2a \right]

  • D

    [a4,3a2]\left[ \frac{a}{4}, \frac{3a}{2} \right]

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: A long straight wire of radius aa carries a steady current II uniformly distributed over its cross-section.

Find: The distances from the centre where the magnetic field is half of the maximum possible magnetic field, once inside the wire and once outside the wire.

For a uniformly distributed current, the magnetic field inside the wire is

B=μ0Ir2πa2B = \frac{\mu_0 I r}{2\pi a^2}

The maximum magnetic field occurs at the surface, that is at r=ar=a:

Bmax=μ0I2πaB_{\max} = \frac{\mu_0 I}{2\pi a}

Half of the maximum value is

Bmax2=μ0I4πa\frac{B_{\max}}{2} = \frac{\mu_0 I}{4\pi a}

Set the inside-field expression equal to this value:

μ0Ir2πa2=μ0I4πa\frac{\mu_0 I r}{2\pi a^2} = \frac{\mu_0 I}{4\pi a}

So,

r=a2r = \frac{a}{2}

Thus, inside the wire, the required distance is a2\frac{a}{2}.

For points outside the wire,

B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}

Again, taking half of the maximum value,

μ0I2πr=μ0I4πa\frac{\mu_0 I}{2\pi r} = \frac{\mu_0 I}{4\pi a}

This gives

r=2ar = 2a

Thus, outside the wire, the required distance is 2a2a.

Therefore, the distances are [a2,2a]\left[ \frac{a}{2}, 2a \right] and the correct option is B.

Note: The solution states "The Correct Option is C", but its working and final value clearly give [a2,2a]\left[ \frac{a}{2}, 2a \right], which matches option B.

Stepwise Derivation

Given: Radius of wire =a= a, current =I= I, and current distribution is uniform.

Find: Where the magnetic field becomes half of its maximum value inside and outside the wire.

  1. Inside the wire, the field varies linearly with distance rr from the centre:
Binside=μ0Ir2πa2B_{\text{inside}} = \frac{\mu_0 I r}{2\pi a^2}
  1. The maximum field anywhere due to the wire occurs at the surface r=ar=a:
Bmax=μ0I2πaB_{\max} = \frac{\mu_0 I}{2\pi a}
  1. Half of this maximum is
12Bmax=μ0I4πa\frac{1}{2}B_{\max} = \frac{\mu_0 I}{4\pi a}
  1. Equating inside field to half maximum,
μ0Ir2πa2=μ0I4πa\frac{\mu_0 I r}{2\pi a^2} = \frac{\mu_0 I}{4\pi a}

Cancelling common terms,

ra2=12a\frac{r}{a^2} = \frac{1}{2a}

Hence,

r=a2r = \frac{a}{2}
  1. Outside the wire, the field is
Boutside=μ0I2πrB_{\text{outside}} = \frac{\mu_0 I}{2\pi r}
  1. Set this equal to half maximum:
μ0I2πr=μ0I4πa\frac{\mu_0 I}{2\pi r} = \frac{\mu_0 I}{4\pi a}

So,

1r=12a\frac{1}{r} = \frac{1}{2a}

Therefore,

r=2ar = 2a

Thus, the required pair is [a2,2a]\left[ \frac{a}{2}, 2a \right], so the correct option is B.

Common mistakes

  • Using the outside-field formula B=μ0I2πrB = \frac{\mu_0 I}{2\pi r} for points inside the wire. This is wrong because inside a uniformly current-carrying wire, only the enclosed current contributes. Use B=μ0Ir2πa2B = \frac{\mu_0 I r}{2\pi a^2} for rar \le a instead.

  • Taking the maximum magnetic field at the centre of the wire. This is incorrect because the inside field increases linearly with rr and becomes maximum at the surface r=ar=a. First identify BmaxB_{\max} correctly before halving it.

  • Following the listed correct option label from the page without checking the algebra. the working label says C, but the worked solution gives r=a2r=\frac{a}{2} inside and r=2ar=2a outside, which matches B. Always trust the derivation over a mismatched label.

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