Question:

The centripetal acceleration of a particle in uniform circular motion is \( 18 \, {ms}^{-2} \). If the radius of the circular path is \( 50 \) cm, the change in velocity of the particle in a time of \( \frac{T}{18} \) is:

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For uniform circular motion, the velocity change over a given time is calculated using the angular displacement and the sine function.
Updated On: Mar 25, 2025
  • \( 9 \, {ms}^{-1} \)
  • \( 2 \, {ms}^{-1} \)
  • \( 3 \, {ms}^{-1} \)
  • \( 6 \, {ms}^{-1} \)
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The Correct Option is C

Solution and Explanation

Step 1: Determine velocity of the particle
The centripetal acceleration is given by: \[ a_c = \frac{v^2}{r} \] Substituting the given values: \[ 18 = \frac{v^2}{0.50} \] \[ v^2 = 18 \times 0.50 = 9 \] \[ v = 3 { ms}^{-1}. \] Step 2: Change in velocity in time \( \frac{T}{18} \)
The time period \( T \) is given by: \[ T = \frac{2\pi r}{v}. \] Substituting \( r = 0.50 \) m and \( v = 3 \) ms\(^{-1}\): \[ T = \frac{2\pi \times 0.50}{3} = \frac{\pi}{3} { s}. \] The time given in the problem is: \[ t = \frac{T}{18} = \frac{\pi}{3} \times \frac{1}{18} = \frac{\pi}{54} { s}. \] The change in velocity for uniform circular motion over time \( t \) is: \[ \Delta v = v \sin \theta. \] Since in a time \( \frac{T}{18} \), the angular displacement is: \[ \theta = \frac{2\pi}{T} \times t = \frac{2\pi}{\pi/3} \times \frac{\pi}{54} = \frac{6}{1} \times \frac{\pi}{54} = \frac{6\pi}{54} = \frac{\pi}{9}. \] Thus, \[ \Delta v = v \sin \frac{\pi}{9}. \] Approximating \( \sin \frac{\pi}{9} \approx 1/3 \): \[ \Delta v = 3 \times \frac{1}{3} = 3 { ms}^{-1}. \] Step 3: Conclusion
Thus, the correct answer is: \[ 3 \, {ms}^{-1}. \]
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