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Question: A current carrying wire is in the form of square loop of side length\(10cm\). Current wire is \(5A\)...

A current carrying wire is in the form of square loop of side length10cm10cm. Current wire is 5A5A . Find the magnetic field at the center of the loop.
(A) 107T{10^{ - 7}}T
(B) 2×107T\sqrt 2 \times {10^{ - 7}}T
(C) 42×105T4\sqrt 2 \times {10^{ - 5}}T
(D) 4×107T4 \times {10^{ - 7}}T

Explanation

Solution

Hint We are given the side of the current carrying square loop and the current flowing through it and are asked to find the magnetic field at the center of the loop. We will use the concepts where we could connect the current at a point to the magnetic field and the length of the loop.
Formula Used
B=μ04πIa(cosθ1+cosθ2)B = \dfrac{{{\mu _0}}}{{4\pi }}\dfrac{I}{a}(\cos {\theta _1} + \cos {\theta _2})
Where, BB is the magnetic field at a point, μ0{\mu _0} is the permeability of open space or vacuum, II is the current flowing through the conductor and aa is the distance of the point from the edge of the conductor. θ1{\theta _1} and θ2{\theta _2} are the angle between the line joining the point with one edge and the edge of the loop.

Complete Step By Step Solution

Here,
We have constructed a line OAOA to the mid of one of the edges of the square.
Now,
As OO is the center of the square, the angles θ1=θ2=π4{\theta _1} = {\theta _2} = \dfrac{\pi }{4} (As edge angle of a square is π2\dfrac{\pi }{2})
Now,
The parameters given are,
Current through the conductor, I=5AI = 5A
Length of each edge, L=10cm=101mL = 10cm = {10^{ - 1}}m
Now,
As per the diagram,
Distance of the edge of the square from the center, a=0.5×101m=5×102ma = 0.5 \times {10^{ - 1}}m = 5 \times {10^{ - 2}}m
And we know,
μ0=4π×107Hm1{\mu _0} = 4\pi \times {10^{ - 7}}H{m^{ - 1}}
Thus, applying the formula B=μ04πIaB = \dfrac{{{\mu _0}}}{{4\pi }}\dfrac{I}{a} , we get
B=4π×107Hm14π×5A5×102m(cosπ4+cosπ4)B = \dfrac{{4\pi \times {{10}^{ - 7}}H{m^{ - 1}}}}{{4\pi }} \times \dfrac{{5A}}{{5 \times {{10}^{ - 2}}m}}\left( {\cos \dfrac{\pi }{4} + \cos \dfrac{\pi }{4}} \right)
Calculating and putting in the value cosπ4=12\cos \dfrac{\pi }{4} = \dfrac{1}{{\sqrt 2 }}, we get
B=2×105TB = \sqrt 2 \times {10^{ - 5}}T
Now, each and every edge will apply the same magnetic field on the center
Thus,
Net magnetic field on the center = 4 ×magnetic field by each edge= 4×BNet{\text{ }}magnetic{\text{ }}field{\text{ }}on{\text{ }}the{\text{ }}center{\text{ }} = {\text{ }}4{\text{ }} \times magnetic{\text{ }}field{\text{ }}by{\text{ }}each{\text{ }}edge = {\text{ }}4 \times B
Hence,
BNet=42×105T{B_{Net}} = 4\sqrt 2 \times {10^{ - 5}}T

Thus, the answer is (C).

Note We multiplied the number of edges with the individual magnetic field of each edge in order to get the net magnetic field on the center. But this was the case of a square where each and every edge has the same dimension. If the loop was of a different shape, then the calculations would have been somewhat different from the one we did. As this loop was a square, it was safe to assume that each edge will apply the same amount of magnetic field on the center.