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A particle moves along a circle of radiu...

A particle moves along a circle of radius r with constant tangential acceleration. If the velocity of the particle is v at the end of second revolution, after the revolution has started, then the tangential acceleration is

A

`v^2/(8pir)`

B

`v^2/(6pir)`

C

`v^2/(4pir)`

D

`v^2/(10pir)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the tangential acceleration of a particle moving along a circular path with a constant tangential acceleration. We know that the particle has a velocity \( v \) at the end of the second revolution. ### Step-by-Step Solution: 1. **Understand the Motion**: - The particle moves along a circular path of radius \( r \) with constant tangential acceleration \( a_t \). - The angular velocity \( \omega \) is related to the tangential velocity \( v \) by the equation: \[ \omega = \frac{v}{r} \] 2. **Identify the Angular Displacement**: - After two complete revolutions, the angular displacement \( \theta \) is given by: \[ \theta = 2 \times 2\pi = 4\pi \text{ radians} \] 3. **Use the Angular Motion Equation**: - We can use the third equation of motion for angular motion: \[ \omega_f^2 = \omega_i^2 + 2\alpha\theta \] - Here, \( \omega_f \) is the final angular velocity, \( \omega_i \) is the initial angular velocity (which is 0 since the particle starts from rest), \( \alpha \) is the angular acceleration, and \( \theta \) is the angular displacement. 4. **Substituting Values**: - Since the initial angular velocity \( \omega_i = 0 \), the equation simplifies to: \[ \omega_f^2 = 2\alpha\theta \] - Substituting \( \theta = 4\pi \): \[ \omega_f^2 = 2\alpha(4\pi) = 8\pi\alpha \] 5. **Relate Angular and Tangential Acceleration**: - The angular acceleration \( \alpha \) is related to the tangential acceleration \( a_t \) by: \[ \alpha = \frac{a_t}{r} \] - Substituting this into the equation gives: \[ \omega_f^2 = 8\pi\left(\frac{a_t}{r}\right) \] 6. **Substituting for Final Angular Velocity**: - We also know that \( \omega_f = \frac{v}{r} \), so substituting this into the equation gives: \[ \left(\frac{v}{r}\right)^2 = 8\pi\left(\frac{a_t}{r}\right) \] 7. **Simplifying the Equation**: - This simplifies to: \[ \frac{v^2}{r^2} = \frac{8\pi a_t}{r} \] - Multiplying both sides by \( r^2 \) gives: \[ v^2 = 8\pi a_t r \] 8. **Solving for Tangential Acceleration**: - Finally, we can solve for the tangential acceleration \( a_t \): \[ a_t = \frac{v^2}{8\pi r} \] ### Final Answer: The tangential acceleration \( a_t \) is: \[ a_t = \frac{v^2}{8\pi r} \]
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