MCQEasyJEE 2024Force on Current-Carrying Conductor

JEE Physics 2024 Question with Solution

A rigid wire consists of a semicircular portion of radius RR and two straight sections. The wire is partially immersed in a perpendicular magnetic field B=B0j^\vec{B} = B_0\,\hat{j}. The magnetic force on the wire if it has a current ii is:

  • A

    iBRj^-iBR\,\hat{j}

  • B

    2iBRj^2iBR\,\hat{j}

  • C

    iBRj^iBR\,\hat{j}

  • D

    2iBRj^-2iBR\,\hat{j}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: A rigid wire has a semicircular portion of radius RR and two straight sections. It carries current ii and is placed in a perpendicular magnetic field B\vec{B}.

Find: The net magnetic force on the wire.

For a current-carrying wire in a uniform magnetic field,

F=iL×B\vec{F} = i\,\vec{L} \times \vec{B}

where L\vec{L} is the effective length vector from one end of the segment to the other.

For the semicircular part, the effective length equals the diameter, so its magnitude is

L=2RL = 2R

The two straight sections are parallel to the magnetic field, so the force on each straight segment is zero.

Fstraight=0\vec{F}_{\text{straight}} = 0

Hence the total force is due to the semicircular part alone. Substituting the effective length 2R2R,

F=i(2R)B\vec{F} = i\,(2R)\,B\,

Using the right-hand rule for the given current direction and magnetic field, the force is along j^-\hat{j}. Therefore,

F=2iBRj^\vec{F} = -2iBR\,\hat{j}

Therefore, the correct option is D.

Use effective length of the arc

Given: Only the portion of wire inside the field contributes to magnetic force.

Find: Net force on the wire.

A wire segment in uniform magnetic field can be treated using the end-to-end vector of that segment:

F=il×B\vec{F} = i\,\vec{l} \times \vec{B}

For a semicircular arc, the end-to-end distance is the diameter,

l=2Rl = 2R

The straight sections are parallel to B\vec{B}, so they contribute no force. Thus directly,

F=i(2R)B\vec{F} = i\,(2R)\,B

With direction from the right-hand rule, the force is j^-\hat{j}. Hence,

F=2iBRj^\vec{F} = -2iBR\,\hat{j}

So the correct option is D.

Common mistakes

  • Treating the arc length as πR\pi R in F=iL×B\vec{F} = i\vec{L} \times \vec{B}. This is wrong because L\vec{L} is the end-to-end vector, not the path length. Use the diameter 2R2R for the semicircular part.

  • Adding force from the straight sections without checking orientation. This is wrong because a wire parallel to the magnetic field has zero magnetic force. First test whether the segment is parallel to B\vec{B}.

  • Getting the magnitude correct but the direction wrong. This happens when the right-hand rule is applied carelessly. Determine the direction from l×B\vec{l} \times \vec{B} before choosing the option.

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