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If the radius of earth contracts 1/n of ...

If the radius of earth contracts 1/n of its present day value, the length of the day will be approximately

A

`(24)/(n)h`

B

`(24)/(n^(2))h`

C

`24 nh`

D

`24 n^(2)h`

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The correct Answer is:
To solve the problem, we need to determine how the length of the day changes when the radius of the Earth contracts to \( \frac{1}{n} \) of its present value. We will use the conservation of angular momentum and the relationship between the moment of inertia, angular velocity, and the period of rotation. ### Step-by-Step Solution: 1. **Understanding the Initial Conditions**: - Let the initial radius of the Earth be \( R \). - The initial time period \( T \) (length of the day) is 24 hours. 2. **Angular Momentum Conservation**: - The angular momentum \( L \) of a rotating body is given by: \[ L = I \cdot \omega \] where \( I \) is the moment of inertia and \( \omega \) is the angular velocity. - For a solid sphere, the moment of inertia \( I \) is: \[ I = \frac{2}{5} m R^2 \] - The angular velocity \( \omega \) is related to the time period \( T \) by: \[ \omega = \frac{2\pi}{T} \] 3. **New Conditions After Radius Contraction**: - When the radius contracts to \( R' = \frac{R}{n} \), we need to find the new time period \( T' \). - The new moment of inertia \( I' \) becomes: \[ I' = \frac{2}{5} m (R')^2 = \frac{2}{5} m \left(\frac{R}{n}\right)^2 = \frac{2}{5} m \frac{R^2}{n^2} \] 4. **Setting Up the Angular Momentum Equation**: - By conservation of angular momentum: \[ L' = L \] which implies: \[ I' \cdot \omega' = I \cdot \omega \] - Substituting the expressions for \( I \) and \( I' \): \[ \left(\frac{2}{5} m \frac{R^2}{n^2}\right) \cdot \omega' = \left(\frac{2}{5} m R^2\right) \cdot \omega \] - Simplifying gives: \[ \frac{R^2}{n^2} \cdot \omega' = R^2 \cdot \omega \] 5. **Solving for the New Angular Velocity**: - Dividing both sides by \( R^2 \): \[ \frac{\omega'}{n^2} = \omega \] - Thus, we find: \[ \omega' = n^2 \cdot \omega \] 6. **Finding the New Time Period**: - Since \( \omega' = \frac{2\pi}{T'} \) and \( \omega = \frac{2\pi}{T} \): \[ \frac{2\pi}{T'} = n^2 \cdot \frac{2\pi}{T} \] - Cancelling \( 2\pi \) from both sides: \[ \frac{1}{T'} = n^2 \cdot \frac{1}{T} \] - Rearranging gives: \[ T' = \frac{T}{n^2} \] 7. **Substituting the Initial Time Period**: - Since \( T = 24 \) hours: \[ T' = \frac{24}{n^2} \text{ hours} \] 8. **Final Answer**: - Therefore, the length of the day after the contraction of the Earth's radius will be: \[ T' = \frac{24}{n^2} \text{ hours} \] ### Conclusion: The correct answer is option 2: \( \frac{24}{n^2} \) hours.

To solve the problem, we need to determine how the length of the day changes when the radius of the Earth contracts to \( \frac{1}{n} \) of its present value. We will use the conservation of angular momentum and the relationship between the moment of inertia, angular velocity, and the period of rotation. ### Step-by-Step Solution: 1. **Understanding the Initial Conditions**: - Let the initial radius of the Earth be \( R \). - The initial time period \( T \) (length of the day) is 24 hours. ...
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