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Question: The magnetic field at the centre of coil of \(n\) turns, bent in the form of a square of side \(2l\)...

The magnetic field at the centre of coil of nn turns, bent in the form of a square of side 2l2l, carrying current ii, is :
A. 2μ0niπl\dfrac{\sqrt{2}{{\mu }_{0}}ni}{\pi l}
B. 2μ0ni2πl\dfrac{\sqrt{2}{{\mu }_{0}}ni}{2\pi l}
C. 2μ0ni4πl\dfrac{\sqrt{2}{{\mu }_{0}}ni}{4\pi l}
D. 2μ0niπl\dfrac{2{{\mu }_{0}}ni}{\pi l}

Explanation

Solution

Use the formula for the magnitude of the magnetic field at a point, which is at a perpendicular distance d from the straight conductor carrying some current. Make use of the symmetry of a square.Magnetic field is an invisible space around a magnetic object. A magnetic field is basically used to describe the distribution of magnetic force around a magnetic object.

Formula used:
B=μ0i4πd(sinθ1+sinθ2)B=\dfrac{{{\mu }_{0}}i}{4\pi d}\left( \sin {{\theta }_{1}}+\sin {{\theta }_{2}} \right)

Complete step by step answer:
It is given that there is coil carrying current i, in the shape of a square. The coils have nn turns and the length of each side of the square is 2l2l. Now, consider a straight conductor carrying current ii of length l. The magnitude of the magnetic field at a point, which is at a perpendicular distance d from the straight conductor (as shown in the figure) is given as B=μ0i4πd(sinθ1+sinθ2)B=\dfrac{{{\mu }_{0}}i}{4\pi d}\left( \sin {{\theta }_{1}}+\sin {{\theta }_{2}} \right) ….. (i).

The direction of the magnetic field is given by the right hand thumb rule.
In the given case, the coil is in the form of a square.

Due to symmetry, the magnitude of the magnetic field produced by each side of the square, at the centre of the coil is the same. From the right hand thumb rule, the direction of the four magnetic field fields will be inwards. Let us calculate the magnetic field due to any one side. In the figure we can see that for each side the angles θ1{{\theta }_{1}} and θ2{{\theta }_{2}} are equal to 45{{45}^{\circ }} each. And the perpendicular distance of the centre from the side is l.
Now, substitute θ1=θ2=45{{\theta }_{1}}={{\theta }_{2}}={{45}^{\circ }} and d=ld=l.
B=μ0i4πl(sin45+sin45)\Rightarrow B=\dfrac{{{\mu }_{0}}i}{4\pi l}\left( \sin {{45}^{\circ }}+\sin {{45}^{\circ }} \right)
B=μ0i4πl(12+12)=μ0i22πl\Rightarrow B=\dfrac{{{\mu }_{0}}i}{4\pi l}\left( \dfrac{1}{\sqrt{2}}+\dfrac{1}{\sqrt{2}} \right)=\dfrac{{{\mu }_{0}}i}{2\sqrt{2}\pi l}.
This means that the magnetic field produced by each side of the square at the centre is equal to B=μ0i22πlB=\dfrac{{{\mu }_{0}}i}{2\sqrt{2}\pi l}
Since the direction of all four magnetic fields is same, the magnetic field produced by one such coil at the centre is equal to 4B=4(μ0i22πl)=2μ0iπl4B=4\left( \dfrac{{{\mu }_{0}}i}{2\sqrt{2}\pi l} \right)=\dfrac{\sqrt{2}{{\mu }_{0}}i}{\pi l}.
It is given that there are nn turns in the coil. Therefore, the net magnetic field at the centre of the coils is equal to 2nμ0iπl\dfrac{\sqrt{2}n{{\mu }_{0}}i}{\pi l}.

Hence, the correct option is A.

Note: In case of a straight current carrying conductor, the right hand thumb rule says that if we point our thumb in the direction of the current flowing in the conductor, then in the direction in which we curl our other figures will give the direction of the magnetic field line.