Step 1: Understanding the Concept:
The time period of a simple pendulum is determined by its effective length and the effective acceleration due to gravity ($g_{eff}$). When immersed in a liquid, the buoyant force reduces the effective weight, thereby reducing $g_{eff}$.
Step 2: Key Formula or Approach:
1. Original Time Period: \( T = 2\pi \sqrt{\frac{l}{g}} \)
2. Effective gravity in liquid: \( g' = g \left( 1 - \frac{\rho_{liquid}}{\rho_{bob}} \right) \)
Step 3: Detailed Explanation:
Given:
- Density of liquid \(\sigma = \frac{1}{4} \rho\) (where \(\rho\) is bob density).
- New length \(l' = l + \frac{l}{3} = \frac{4l}{3}\).
First, calculate the effective acceleration due to gravity (\(g'\)) in the liquid:
\[ g' = g \left( 1 - \frac{\sigma}{\rho} \right) = g \left( 1 - \frac{1/4 \rho}{\rho} \right) = g \left( 1 - \frac{1}{4} \right) = \frac{3g}{4} \]
Now, calculate the new time period \(T'\):
\[ T' = 2\pi \sqrt{\frac{l'}{g'}} = 2\pi \sqrt{\frac{4l/3}{3g/4}} \]
\[ T' = 2\pi \sqrt{\frac{4l}{3} \times \frac{4}{3g}} = 2\pi \sqrt{\frac{16l}{9g}} \]
\[ T' = \frac{4}{3} \times 2\pi \sqrt{\frac{l}{g}} \]
Since \(T = 2\pi \sqrt{l/g}\), we get:
\[ T' = \frac{4}{3} T \]
Step 4: Final Answer:
The new time period is \(\frac{4}{3} T\).