A current \( i \) flows through a circular loop of radius \( R \). The ratio of the magnetic field produced at its centre to the field produced at a point at a distance \( \frac{R}{\sqrt{3}} \) from its centre on its axis is:
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The magnetic field at the center of a current-carrying loop is stronger than the field at a point on its axis, with the strength decreasing as we move away from the center.
Step 1: The magnetic field at the center of the loop is given by:
\[
B_{\text{center}} = \frac{\mu_0 i}{2R}
\]
where \( i \) is the current and \( R \) is the radius of the loop.
Step 2: The magnetic field at a distance \( \frac{R}{\sqrt{3}} \) on the axis of the loop is given by:
\[
B_{\text{axis}} = \frac{\mu_0 i}{4R} \left( \frac{1}{\left( 1 + \left(\frac{d}{R}\right)^2 \right)^{3/2}} \right)
\]
Step 3: The ratio of the magnetic fields is:
\[
\frac{B_{\text{center}}}{B_{\text{axis}}} = 8:1
\]