MCQMediumJEE 2026Biot–Savart Law

JEE Physics 2026 Question with Solution

An infinitely long straight wire carrying current II is bent in a planar shape as shown in the diagram. The radius of the circular part is rr. The magnetic field at the centre OO of the circular loop is :

A straight horizontal wire segment with points A, B, D, and E marked, bent into a circular loop above the wire touching near B and D, center O shown with radius r to the loop, current I indicated along the wire and loop, and axes labeled x, y, z near the right side.
  • A

    μ0I2πr(π1)i^\frac{\mu_0 I}{2 \pi r} (\pi - 1) \hat{i}

  • B

    μ0I2πr(π+1)i^\frac{\mu_0 I}{2 \pi r} (\pi + 1) \hat{i}

  • C

    μ0I2πr(π1)i^-\frac{\mu_0 I}{2 \pi r} (\pi - 1) \hat{i}

  • D

    μ0I2πr(π+1)i^-\frac{\mu_0 I}{2 \pi r} (\pi + 1) \hat{i}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: An infinitely long straight wire carrying current II is bent to form a circular loop of radius rr and a straight wire segment in the same plane.

Find: The magnetic field at the centre OO of the circular loop.

The total magnetic field at OO is the vector sum of the fields due to the circular loop and the infinitely long straight wire.

Field due to the circular loop at its centre:

Bloop=μ0I2rB_{\text{loop}} = \frac{\mu_0 I}{2r}

Field due to an infinitely long straight wire at distance rr:

Bwire=μ0I2πrB_{\text{wire}} = \frac{\mu_0 I}{2 \pi r}

Based on the current direction in the diagram, the current in the loop is counter-clockwise, so by the right-hand thumb rule the magnetic field at OO is out of the page, corresponding here to i^\hat{i}.

The straight wire also produces a magnetic field at OO in the same direction, so the two fields add.

Therefore,

Bnet=Bloop+Bwire\vec{B}_{\text{net}} = \vec{B}_{\text{loop}} + \vec{B}_{\text{wire}} Bnet=(μ0I2r+μ0I2πr)i^\vec{B}_{\text{net}} = \left( \frac{\mu_0 I}{2r} + \frac{\mu_0 I}{2 \pi r} \right) \hat{i} Bnet=μ0I2πr(π+1)i^\vec{B}_{\text{net}} = \frac{\mu_0 I}{2 \pi r}(\pi + 1) \hat{i}

Therefore, the correct option is B.

Direction Check with Right-Hand Thumb Rule

Given: The magnetic field at the centre OO is produced by both the circular part and the straight part of the current-carrying wire.

Find: Whether the two contributions add or subtract.

Use the right-hand thumb rule separately for each segment:

  1. For the circular loop, the current is counter-clockwise, so the field at the centre is directed out of the plane.
  2. For the straight wire, at the point OO located a distance rr above the wire, the field is also out of the plane in the given coordinate convention, that is along i^\hat{i}.

Since both magnetic fields are along the same direction, they reinforce each other.

Hence,

Bnet=μ0I2ri^+μ0I2πri^\vec{B}_{\text{net}} = \frac{\mu_0 I}{2r}\hat{i} + \frac{\mu_0 I}{2 \pi r}\hat{i} Bnet=μ0I2πr(π+1)i^\vec{B}_{\text{net}} = \frac{\mu_0 I}{2 \pi r}(\pi + 1)\hat{i}

So the magnetic field is μ0I2πr(π+1)i^\frac{\mu_0 I}{2 \pi r}(\pi + 1)\hat{i}.

Common mistakes

  • Adding the magnitudes without checking direction is incorrect because magnetic field is a vector quantity. First use the right-hand thumb rule for both the loop and the straight wire, then decide whether to add or subtract.

  • Using the straight-wire formula for the circular loop is wrong because the field at the centre of a full circular loop is μ0I2r\frac{\mu_0 I}{2r}, not μ0I2πr\frac{\mu_0 I}{2 \pi r}. Use the correct expression for each segment separately.

  • Choosing the negative sign by assuming the field goes into the page is a direction error. The current sense shown gives the field at OO along positive i^\hat{i}, so the net field is positive in that direction.

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