Question 18

NUMERICALHARD

Rotational Dynamics of a Pivoted Circular Disk and Particle Collision

A uniform circular disk of radius 0.2 m0.2 \text{ m} and mass 1 kg1 \text{ kg} is pivoted at its top point CC such that it can rotate freely around CC in the XYXY plane, as shown in the figure. Initially, when the disk is at rest, a particle of mass 20 g20 \text{ g}, travelling along negative xx direction in the XYXY plane with speed 100 ms−1100 \text{ ms}^{-1}, hits the circumference of the disk at a point PP. After collision the particle moves along negative yy direction at a speed of 90 ms−190 \text{ ms}^{-1}. [Given: the acceleration due to gravity (g)=−10j^ ms−2(g) = - 10 \hat{j} \text{ ms}^{-2}]

Passage

Amount of energy loss (in J) in the collision is:

Correct Answer: 17.5

Detailed Solution

  1. Initial Kinetic Energy: Ki=12mv12=0.5×0.02×(100)2=100 JK_i = \frac{1}{2} m v_1^2 = 0.5 \times 0.02 \times (100)^2 = 100 \text{ J}.

  2. Final Kinetic Energy: Kf,particle=12mv22=0.5×0.02×(90)2=81 JK_{f, particle} = \frac{1}{2} m v_2^2 = 0.5 \times 0.02 \times (90)^2 = 81 \text{ J}. Kf,disk=12ICω2K_{f, disk} = \frac{1}{2} I_C \omega^2 (from previous question calculation) ≈1.528 J\approx 1.528 \text{ J}. Total Kf=81+1.528=82.528 JK_f = 81 + 1.528 = 82.528 \text{ J}.

  3. Energy Loss: Loss =Ki−Kf=100−82.528=17.472 J= K_i - K_f = 100 - 82.528 = 17.472 \text{ J}. Rounding to one decimal place, we get 17.5 J17.5 \text{ J}.

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