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Physics · SYSTEMS OF PARTICLES AND ROTATIONAL MOTION

हिन्दी

When a bicycle rim is suspended vertically by two strings at the axle ends and made to rotate rapidly, releasing one of the strings causes the axle of rotation to:

  1. immediately fall downward and stop rotating completely.
  2. accelerate linearly upward due to the reaction torque.
  3. remain stationary in its initial horizontal orientation without any tilt.
  4. precess about the vertical string supporting the other end.

Correct answer · Option 4

precess about the vertical string supporting the other end.

Explanation

The gravitational torque acts perpendicular to both the angular momentum and the vertical axis, causing the angular momentum and the axis of the rotating rim to precess around the remaining supporting string.

Related questions

Given below are two statements: Statement I: The kinetic energy of a body of moment of inertia \( I \) rotating with an angular velocity \( \omega \) about a fixed axis is given by \( K = \frac{1}{2} I \omega^2 \). Statement II: The moment of inertia of a rotating rigid body changes if its angular velocity is doubled. In the light of the above statements, choose the most appropriate answer from the options given below:→Given two vectors \( \mathbf{a} = 3\hat{i} - 4\hat{j} + 5\hat{k} \) and \( \mathbf{b} = -2\hat{i} + \hat{j} - 3\hat{k} \), the cross product \( \mathbf{a} \times \mathbf{b} \) is equal to:→Consider the following statements regarding rotational motion about a fixed axis: (A) Only those components of external torques that lie along the axis of rotation can cause the body to rotate about the axis. (B) Torques perpendicular to the fixed axis are balanced by the constraint forces exerted by the hinges/supports. (C) Forces parallel to the axis of rotation produce non-zero torque about that axis. (D) The rate of work done by an external torque \( \tau \) rotating a body with angular speed \( \omega \) is given by \( P = \tau \omega \). How many of the above statements are correct?→In an L-shaped uniform lamina formed by three identical squares of side length \( b = 2\text{ m} \) as oriented in Fig. 6.11 (with bottom-left square at origin having vertices from \( (0,0) \) to \( (2,2) \)), the coordinate of the centre of mass is:→
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