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In the above problem, if the rod is rele...

In the above problem, if the rod is released from horizontal position, the angular velocity of the rod as it passes the vertical position is (l=length fo rod)

A

`sqrt((12g)/(5l))`

B

`sqrt((2g)/(3l))`

C

`sqrt((3g)/(l))`

D

`sqrt((3g)/(7l))`

Text Solution

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The correct Answer is:
To solve the problem of finding the angular velocity of a rod as it passes the vertical position after being released from a horizontal position, we can follow these steps: ### Step-by-Step Solution: 1. **Identify the System**: - We have a uniform rod of length \( l \) that is hinged at one end and initially held in a horizontal position. 2. **Determine the Initial and Final Positions**: - The initial position of the rod is horizontal, and the final position we are interested in is vertical. 3. **Calculate the Change in Potential Energy**: - The center of mass of the rod is located at a distance of \( \frac{l}{2} \) from the hinge. - When the rod is horizontal, its height relative to the lowest point (vertical position) is \( \frac{l}{2} \). - The loss in gravitational potential energy (PE) as the rod moves from horizontal to vertical is given by: \[ \Delta PE = mgh = mg \cdot \frac{l}{2} \] 4. **Relate Potential Energy to Kinetic Energy**: - As the rod falls, the loss in potential energy is converted into kinetic energy (KE). - The kinetic energy of a rotating body is given by: \[ KE = \frac{1}{2} I \omega^2 \] - For a rod rotating about one end, the moment of inertia \( I \) is: \[ I = \frac{1}{3} ml^2 \] 5. **Set Up the Energy Conservation Equation**: - Equating the loss in potential energy to the gain in kinetic energy: \[ mg \cdot \frac{l}{2} = \frac{1}{2} \left(\frac{1}{3} ml^2\right) \omega^2 \] 6. **Simplify the Equation**: - Cancel \( m \) from both sides (assuming \( m \neq 0 \)): \[ g \cdot \frac{l}{2} = \frac{1}{6} l^2 \omega^2 \] - Multiply both sides by 6: \[ 3gl = l^2 \omega^2 \] 7. **Solve for Angular Velocity \( \omega \)**: - Rearranging gives: \[ \omega^2 = \frac{3g}{l} \] - Taking the square root: \[ \omega = \sqrt{\frac{3g}{l}} \] 8. **Final Result**: - The angular velocity of the rod as it passes the vertical position is: \[ \omega = \sqrt{\frac{3g}{l}} \] ### Conclusion: The correct answer is option C: \( \sqrt{\frac{3g}{l}} \).
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