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Question: A conducting wire bent in the form of a parabola \[{y^2} = 2x\] carries a current \[i = 2{\text{ A}}...

A conducting wire bent in the form of a parabola y2=2x{y^2} = 2x carries a current i=2 Ai = 2{\text{ A}} as shown in figure. This wire is placed in a uniform magnetic field B=4k\overrightarrow B = 4\overrightarrow k Tesla. The magnetic force on the wire in region 0<x<2m0 < x < 2m is (in Newtons)
A. 16i^ - 16\widehat i
B. 32i^32\widehat i
C. 32i^ - 32\widehat i
D. 16i^16\widehat i

Explanation

Solution

When a current-carrying conductor is placed in a magnetic field, then the conductor experiences a force in a direction perpendicular to both the directions of the magnetic field and the direction of current flowing in the conductor. If the magnetic field is uniform, the magnetic force for an arbitrary shape wire can be written as F=i(l×B)F = i\left( {l \times B} \right) where ll is the effective length of the arbitrary wire.

Formula used:
Magnetic force on a current carrying conductor,
F=dF=i(dl×B)F = \int {dF = } i\left( {\int d l \times B} \right)
If the magnetic field is uniform,
Magnetic force can be written as,
F=i(l×B)F = i\left( {l \times B} \right)
where ll is the effective length of the arbitrary wire, BB is the uniform magnetic field and ii is the current in the conductor.

Complete step by step answer:
We are given, a conducting wire bent in the form of a parabola y2=2x{y^2} = 2x carries a current i=2 Ai = 2{\text{ A}}. The Magnetic field present is B=4k\overrightarrow B = 4\overrightarrow k Tesla. We need to find the magnetic force on the wire. Magnetic force on a current carrying conductor is given by,
F=dF=i(dl×B)F = \int {dF = } i\left( {\int d l \times B} \right)

Coordinates of point AA is (2,2)\left( {2,2} \right) and coordinates of point BB is (2,2)\left( {2, - 2} \right). Therefore, the effective length of the conducting wire will be length of ABAB i.e.,4 m4{\text{ m}}. Since, the current is flowing from point AA to point BB therefore, current in the imaginary conductor will also flow from point AA to point BB in j^ - \widehat j direction. If the magnetic field is uniform, magnetic force becomes,
F=i(l×B)F = i\left( {l \times B} \right)
where ll is the effective length of the arbitrary wire.

Substituting the values in the equation,
F=2×((4j^)×(4k^))F = 2 \times \left( {\left( { - 4\widehat j} \right) \times \left( {4\widehat k} \right)} \right)
After performing the cross product, we get,
F=2×16i^F = 2 \times - 16\widehat i
F=32i^\therefore F = - 32\widehat i
Thus, the magnetic force acting on the current-carrying inductor is equal to 32i^ - 32\widehat i.

Thus, option C is the correct answer.

Note: Magnetic force on the conductor will be maximum when it is placed perpendicular to the magnetic field and force on the conductor will be zero when it is placed parallel to the magnetic field. Force on a closed current-carrying loop in a uniform magnetic field is also zero.