\[ B_{\text{center}} = \frac{\mu_0 I}{2R} \]
The magnetic field at a point on the axis of a current-carrying circular coil is:
\[ B_x = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}} \]
We are told:
\[ B_{\text{center}} = 64 \cdot B_x \] Substituting both expressions: \[ \frac{\mu_0 I}{2R} = 64 \cdot \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}} \]
Cancel \( \frac{\mu_0 I}{2} \) on both sides:
\[ \frac{1}{R} = 64 \cdot \frac{R^2}{(R^2 + x^2)^{3/2}} \Rightarrow \frac{1}{R} = \frac{64R^2}{(R^2 + x^2)^{3/2}} \]
\[ (R^2 + x^2)^{3/2} = 64R^3 \Rightarrow R^2 + x^2 = (64R^3)^{2/3} = 16R^2 \Rightarrow x^2 = 15R^2 \Rightarrow x = R\sqrt{15} \]
The value of \( x \) is \( \boxed{R\sqrt{15}} \), so the correct answer is (D).
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:

An infinite wire has a circular bend of radius \( a \), and carrying a current \( I \) as shown in the figure. The magnitude of the magnetic field at the origin \( O \) of the arc is given by: