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A uniform stick of length l is mounted s...

A uniform stick of length `l` is mounted so as to rotate about a horizontal axis perpendicular to the stick and at a distance `d` from the centre of mass. The time period of small oscillation has a minimum value when `d//l` is

A

`(a)(1)/(sqrt(2)`

B

`(b)(1)/sqrt(12)`

C

`(c)(1)/sqrt(3)`

D

`(d)(1)/sqrt (6)`

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The correct Answer is:
To solve the problem of finding the ratio \( \frac{d}{l} \) for the minimum time period of small oscillations of a uniform stick, we will follow these steps: ### Step 1: Understand the Problem We have a uniform stick of length \( l \) that is rotating about a horizontal axis perpendicular to the stick, at a distance \( d \) from its center of mass. We need to find the ratio \( \frac{d}{l} \) when the time period of small oscillations is minimized. ### Step 2: Write the Formula for Time Period The time period \( T \) of a physical pendulum is given by the formula: \[ T = 2\pi \sqrt{\frac{I}{mgd}} \] where: - \( I \) is the moment of inertia about the suspension point, - \( m \) is the mass of the stick, - \( g \) is the acceleration due to gravity, - \( d \) is the distance from the suspension point to the center of mass. ### Step 3: Calculate the Moment of Inertia The moment of inertia \( I \) of a uniform stick about its center of mass is: \[ I_{cm} = \frac{ml^2}{12} \] When the stick is rotated about a point \( d \) distance away from the center of mass, we use the parallel axis theorem: \[ I = I_{cm} + md^2 = \frac{ml^2}{12} + md^2 \] ### Step 4: Substitute into the Time Period Formula Substituting \( I \) into the time period formula, we get: \[ T = 2\pi \sqrt{\frac{\frac{ml^2}{12} + md^2}{mgd}} \] This simplifies to: \[ T = 2\pi \sqrt{\frac{l^2}{12g d} + \frac{d}{g}} \] ### Step 5: Simplify the Expression We can factor out \( d \) from the square root: \[ T = 2\pi \sqrt{\frac{1}{g} \left( \frac{l^2}{12d} + 1 \right)} \] ### Step 6: Find the Minimum Time Period To find the minimum time period, we need to minimize the expression inside the square root: \[ \frac{l^2}{12d} + 1 \] To do this, we can differentiate with respect to \( d \) and set the derivative to zero: \[ \frac{d}{dd}\left(\frac{l^2}{12d} + 1\right) = -\frac{l^2}{12d^2} = 0 \] This gives us: \[ l^2 = 12d \] Thus, we can express \( d \) in terms of \( l \): \[ d = \frac{l^2}{12} \] ### Step 7: Calculate the Ratio \( \frac{d}{l} \) Now we can find the ratio: \[ \frac{d}{l} = \frac{\frac{l^2}{12}}{l} = \frac{l}{12} \] ### Step 8: Final Result To express this in terms of \( l \): \[ \frac{d}{l} = \frac{1}{12} \] ### Conclusion The minimum value of \( \frac{d}{l} \) when the time period of small oscillation is minimized is: \[ \frac{d}{l} = \frac{1}{\sqrt{12}} \]

To solve the problem of finding the ratio \( \frac{d}{l} \) for the minimum time period of small oscillations of a uniform stick, we will follow these steps: ### Step 1: Understand the Problem We have a uniform stick of length \( l \) that is rotating about a horizontal axis perpendicular to the stick, at a distance \( d \) from its center of mass. We need to find the ratio \( \frac{d}{l} \) when the time period of small oscillations is minimized. ### Step 2: Write the Formula for Time Period The time period \( T \) of a physical pendulum is given by the formula: \[ ...
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