Concept:
A vibration magnetometer works on the principle of a magnetic dipole oscillating in a uniform external magnetic field. The motion is Simple Harmonic Motion (SHM) provided the angular displacement is small.
• Time Period (\(T\)): The time taken for one complete oscillation. It is related to the moment of inertia (\(I\)), magnetic moment (\(M\)), and magnetic field (\(B\)) by the formula:
\[ T = 2\pi \sqrt{\frac{I}{MB}} \]
• Rearranging for \(M\): To find the magnetic moment, we square both sides and rearrange:
\[ T^2 = 4\pi^2 \frac{I}{MB} \implies M = \frac{4\pi^2 I}{T^2 B} \]
Step 1: Calculate the Time Period (\(T\)).
The magnet makes 20 oscillations in 15 seconds.
\[ T = \frac{\text{Total Time}}{\text{Number of oscillations}} = \frac{15}{20} = 0.75 \text{ s} \]
Alternatively, in fractional form for easier calculation: \( T = \frac{3}{4} \text{ s} \).
Step 2: Substitute values into the rearranged formula.
Given:
- \( I = 9 \times 10^{-5} \text{ kg m}^2 \)
- \( B = 16\pi^2 \times 10^{-5} \text{ T} \)
- \( T = 3/4 \text{ s} \) (so \( T^2 = 9/16 \))
\[ M = \frac{4\pi^2 (9 \times 10^{-5})}{\left( \frac{9}{16} \right) (16\pi^2 \times 10^{-5})} \]
Step 3: Simplify and solve for \(M\).
Canceling the terms \(\pi^2\), \(10^{-5}\), and \(9\):
\[ M = \frac{4 \times 1}{\left( \frac{1}{16} \right) \times 16} \]
\[ M = \frac{4}{1} = 4 \text{ Am}^2 \]
*(Note: Re-calculating based on standard options; let's verify numerical simplification.)*
If \( M = \frac{4\pi^2 \times 9 \times 10^{-5}}{\frac{9}{16} \times 16\pi^2 \times 10^{-5}} = \frac{36\pi^2 \times 10^{-5}}{9\pi^2 \times 10^{-5}} = 4 \text{ Am}^2 \).
Option (E) is the correct match.