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A simple pendulum with iron bob has a ti...

A simple pendulum with iron bob has a time period T. The bob is now immersed in a non-viscous liquid and oscillated, if the density of liquid is `(1)/(12)`th that of iron, then new time period will be

A

`T sqrt((8)/(7))`

B

`T sqrt((12)/(13))`

C

`T sqrt((12)/(11))`

D

`T sqrt((6)/(5))`

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The correct Answer is:
To solve the problem, we need to determine the new time period of a simple pendulum bob when it is immersed in a non-viscous liquid with a density that is \( \frac{1}{12} \) of the density of iron. ### Step-by-Step Solution: 1. **Understand the Initial Conditions**: - Let the density of iron be \( \rho_i \). - The density of the liquid is given as \( \rho_l = \frac{1}{12} \rho_i \). - The time period of the pendulum in air is \( T = 2\pi \sqrt{\frac{L}{g}} \), where \( L \) is the length of the pendulum and \( g \) is the acceleration due to gravity. 2. **Calculate the Effective Gravity**: - When the bob is immersed in the liquid, the effective gravity \( g_{\text{effective}} \) is modified due to the buoyant force acting on the bob. - The buoyant force \( F_b \) can be calculated using Archimedes' principle: \( F_b = \rho_l \cdot V \cdot g \), where \( V \) is the volume of the bob. - The weight of the bob \( W \) is given by \( W = \rho_i \cdot V \cdot g \). - The effective weight acting on the bob when submerged is \( W - F_b = \rho_i \cdot V \cdot g - \rho_l \cdot V \cdot g \). 3. **Express the Effective Gravity**: - The effective weight can be expressed as: \[ \text{Effective Weight} = \left( \rho_i - \rho_l \right) V g \] - Substituting \( \rho_l = \frac{1}{12} \rho_i \): \[ \text{Effective Weight} = \left( \rho_i - \frac{1}{12} \rho_i \right) V g = \left( \frac{11}{12} \rho_i \right) V g \] - The effective gravity \( g_{\text{effective}} \) is then: \[ g_{\text{effective}} = \frac{11}{12} g \] 4. **Calculate the New Time Period**: - The new time period \( T' \) of the pendulum in the liquid can be calculated using the formula: \[ T' = 2\pi \sqrt{\frac{L}{g_{\text{effective}}}} \] - Substituting \( g_{\text{effective}} = \frac{11}{12} g \): \[ T' = 2\pi \sqrt{\frac{L}{\frac{11}{12} g}} = 2\pi \sqrt{\frac{12L}{11g}} = \sqrt{\frac{12}{11}} \cdot T \] 5. **Final Result**: - Therefore, the new time period when the bob is immersed in the liquid is: \[ T' = T \sqrt{\frac{12}{11}} \]
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