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# A symmetric star conducting wire loop is carrying a steady current $I$ as shown in the figure. The distance between the diametrically opposite vertices of the star is $4a$. The magnitude of the magnetic field at the center of the loop is(A) $\dfrac{{{\mu _0}I}}{{4\pi a}}6\left( {\sqrt 3 - 1} \right)$(B) $\dfrac{{{\mu _0}I}}{{4\pi a}}6\left( {\sqrt 3 + 1} \right)$(C) $\dfrac{{{\mu _0}I}}{{4\pi a}}3\left( {\sqrt 3 - 1} \right)$(D) $\dfrac{{{\mu _0}I}}{{4\pi a}}3\left( {2 - \sqrt 3 } \right)$

Last updated date: 19th Sep 2024
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Hint We have a conductor in the shape of a symmetric star. The current $I$ is flowing through the conductor. We know that there will be a magnetic field associated with the charges moving through a conductor. The total length between two diametrically opposite vertices of the star is given and we have to find the magnitude of the magnetic field at the center of the star.

According to the right-hand thumb rule, the magnetic field due to the star-shaped current-carrying conductor will be in the upward direction. Since there are $6$ vertices, and each vertex has two sides the total magnetic field will be $12$ times the field due to one side.

Let us consider any one of the sides as $AB$.

The field at a point $O$ can be obtained by joining $A$ and $B$ as shown in the figure.
The dotted lines show the normal perpendicular to the point $O$.
The general formula for the field at the point $O$can be written as,
$B = \dfrac{{{\mu _0}I}}{{4\pi a}}\left( {\sin \alpha - \sin \beta } \right)$
From the above two diagrams, we get
$\alpha = {60^ \circ }$ and $\beta = {30^ \circ }$
Where $B$ stands for the magnetic field, ${\mu _0}$ stands for the permeability of free space, $I$ stands for the current, $a$ stands for the distance between the conductor and the point where we have to find the electric field, and $\alpha$and $\beta$ are the angles as shown in the figure.
Let us assume that the field due to the side $AB$ at the center of the star is ${B_{1.}}$
The field ${B_1}$ can be written as,
${B_1} = \dfrac{{{\mu _0}I}}{{4\pi a}}\left( {\sin {{60}^ \circ } - \sin {{30}^ \circ }} \right)$
We know that $\sin {60^ \circ } = \dfrac{{\sqrt 3 }}{2}$and $\sin {30^ \circ } = \dfrac{1}{2}$
Substituting the value, we get
${B_1} = \dfrac{{{\mu _0}I}}{{4\pi a}}\left( {\dfrac{{\sqrt 3 }}{2} - \dfrac{1}{2}} \right)$
This is the magnetic field due to one side of the star.
We know that the total magnetic field at the center of the star will be $12$ times ${B_1}$
Therefore, we can write the total magnetic field at the center of the star will be,
$B = 12 \times \dfrac{{{\mu _0}I}}{{4\pi a}}\left( {\dfrac{{\sqrt 3 }}{2} - \dfrac{1}{2}} \right)$
This will be,
$B = \dfrac{{{\mu _0}I}}{{4\pi a}}6\left( {\sqrt 3 - 1} \right)$

The answer is: Option (A): $\dfrac{{{\mu _0}I}}{{4\pi a}}6\left( {\sqrt 3 - 1} \right)$

Note
The strength of the magnetic field will be directly proportional to the current through the conductor. The magnetic field will also depend on the length of the conductor that we consider. It is also proportional to the sine angle between the element in the direction of current and the line joining the element and the point of consideration. The magnetic field is inversely proportional to the distance between the conductor and the point of consideration.