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A simple pendulum oscillating in air has...

A simple pendulum oscillating in air has period T. The bob of the pendulum is completely immersed in a non-viscours liquid. The density of the liquid is `(1)/(16)th` of the material of the bob. If the bob is inside liquid all the time, its period of scillation in this liquid is :

A

`2Tsqrt((1)/(10))`

B

`2Tsqrt((1)/(14))`

C

`4Tsqrt((1)/(15))`

D

`4Tsqrt(1)/(14)`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the new period of oscillation \( T' \) of a simple pendulum bob that is completely immersed in a non-viscous liquid, given that the density of the liquid is \( \frac{1}{16} \) of the density of the bob. ### Step-by-Step Solution: 1. **Understanding the Period of a Simple Pendulum:** The period \( T \) of a simple pendulum in air is given by the formula: \[ T = 2\pi \sqrt{\frac{L}{g}} \] where \( L \) is the length of the pendulum and \( g \) is the acceleration due to gravity. 2. **Forces Acting on the Bob in Liquid:** When the bob is immersed in the liquid, the forces acting on it include: - The weight of the bob \( mg \) acting downwards. - The buoyant force \( F_b \) acting upwards, which can be calculated using Archimedes' principle. 3. **Calculating the Buoyant Force:** The buoyant force \( F_b \) is given by: \[ F_b = \text{Volume of bob} \times \text{Density of liquid} \times g \] Since the volume of the bob \( V \) is the same when it is in air and in the liquid, we can express the buoyant force as: \[ F_b = V \cdot \rho_{liquid} \cdot g \] Given that the density of the liquid \( \rho_{liquid} = \frac{1}{16} \rho_{bob} \), we can substitute this into the equation. 4. **Expressing the Mass of the Bob and Liquid:** The mass of the bob is: \[ m = V \cdot \rho_{bob} \] The mass of the liquid displaced by the bob is: \[ m_{liquid} = V \cdot \rho_{liquid} = V \cdot \left(\frac{1}{16} \rho_{bob}\right) \] 5. **Net Force on the Bob:** The net force acting on the bob when it is submerged is: \[ F_{net} = mg - F_b = mg - m_{liquid}g = mg - \left(\frac{1}{16} mg\right) = mg \left(1 - \frac{1}{16}\right) = mg \left(\frac{15}{16}\right) \] 6. **Effective Gravity in Liquid:** The effective gravitational force acting on the bob in the liquid can be defined as: \[ g' = g \left(\frac{15}{16}\right) \] 7. **Finding the New Period of Oscillation:** The new period \( T' \) of the pendulum in the liquid can be expressed as: \[ T' = 2\pi \sqrt{\frac{L}{g'}} \] Substituting \( g' \): \[ T' = 2\pi \sqrt{\frac{L}{g \left(\frac{15}{16}\right)}} = 2\pi \sqrt{\frac{16L}{15g}} = \frac{2\pi}{\sqrt{15}} \sqrt{16L} \] Since \( T = 2\pi \sqrt{\frac{L}{g}} \), we can express \( T' \) in terms of \( T \): \[ T' = T \cdot \frac{4}{\sqrt{15}} \] 8. **Final Result:** Thus, the period of oscillation of the pendulum bob in the liquid is: \[ T' = 4T \cdot \frac{1}{\sqrt{15}} \] ### Final Answer: \[ T' = 4T \cdot \frac{1}{\sqrt{15}} \]
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