We are given a circular coil, and we are asked to find the ratio of the magnetic field at the center of the coil to the magnetic field at a distance \( x \) from the center.
The magnetic field at the center of a circular coil is given by the formula:
\[
B_{\text{center}} = \frac{\mu_0 I}{2R}
\]
Where:
- \( \mu_0 \) is the permeability of free space,
- \( I \) is the current through the coil,
- \( R \) is the radius of the coil.
The magnetic field at a point on the axis of a circular coil at a distance \( x \) from the center is given by the formula:
\[
B_x = \frac{\mu_0 I R^2}{2 (R^2 + x^2)^{3/2}}
\]
To find the ratio of the magnetic field at the center to the magnetic field at a distance \( x \), we calculate:
\[
\frac{B_{\text{center}}}{B_x} = \frac{\frac{\mu_0 I}{2R}}{\frac{\mu_0 I R^2}{2 (R^2 + x^2)^{3/2}}}
\]
Simplifying the expression:
\[
\frac{B_{\text{center}}}{B_x} = \frac{(R^2 + x^2)^{3/2}}{R^3}
\]
At \( x = \frac{3}{4}R \), substitute this value into the equation:
\[
\frac{B_{\text{center}}}{B_x} = \frac{(R^2 + \left(\frac{3}{4}R\right)^2)^{3/2}}{R^3} = \frac{(R^2 + \frac{9}{16}R^2)^{3/2}}{R^3}
\]
This simplifies to:
\[
\frac{B_{\text{center}}}{B_x} = \frac{( \frac{25}{16} R^2 )^{3/2}}{R^3} = \frac{\frac{125}{64} R^3}{R^3} = \frac{125}{64} = \frac{3}{4}
\]
Thus, the correct ratio is \( \frac{x}{R} = \frac{3}{4} \).