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A current I flows in the anticlockwise direction through a square loop of side a lying in the xoy plane with its center at the origin. The magnetic induction at the center of the square loop is
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Verified Answer
The correct answer is:
$\frac{2 \sqrt{2} \mu_{0} I}{\pi a} \hat{e}_{z}$
Field due to one side of loop at $O$
$$
=\frac{\mu_{0} I}{4 \pi\left(\frac{a}{2}\right)}\left(2 \sin 45^{\circ}\right)
$$
Field at $O$ due to all four sides is along unit vector $\hat{e}_{z}$

$\therefore$ Total field
$=4 \cdot \frac{\mu_{0} I}{4 \pi\left(\frac{a}{2}\right)}\left(2 \sin 45^{\circ}\right)=\frac{2 \sqrt{2} \mu_{0} I}{\pi a}$
$$
=\frac{\mu_{0} I}{4 \pi\left(\frac{a}{2}\right)}\left(2 \sin 45^{\circ}\right)
$$
Field at $O$ due to all four sides is along unit vector $\hat{e}_{z}$

$\therefore$ Total field
$=4 \cdot \frac{\mu_{0} I}{4 \pi\left(\frac{a}{2}\right)}\left(2 \sin 45^{\circ}\right)=\frac{2 \sqrt{2} \mu_{0} I}{\pi a}$
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