To solve the given problem, we need to determine the ratio \(\frac{B_1}{B_2}\) using the information about the oscillations of a magnetic dipole in two different magnetic fields.
The frequency of oscillation \(f\) of a magnetic dipole in a magnetic field \(B\) is given by the formula:
\(f = \frac{1}{T} = \frac{1}{2\pi} \sqrt{\frac{\mu B}{I}}\)
where:
For the first scenario in the magnetic field \(B_1\):
Substituting into the frequency formula, we have:
\(\frac{1}{2\pi} \sqrt{\frac{\mu B_1}{I}} = 3\)
For the second scenario in the magnetic field \(B_2\):
Substituting into the frequency formula, we have:
\(\frac{1}{2\pi} \sqrt{\frac{\mu B_2}{I}} = 2\)
Divide the equation for \(f_1\) by the equation for \(f_2\):
\(\frac{3}{2} = \sqrt{\frac{B_1}{B_2}}\)
Squaring both sides to eliminate the square root:
\(\left(\frac{3}{2}\right)^2 = \frac{B_1}{B_2}\)
\(\frac{B_1}{B_2} = \frac{9}{4}\)
Thus, the correct answer is: \(\frac{9}{4}\), which matches the given correct option.
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.