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Physics · SYSTEMS OF PARTICLES AND ROTATIONAL MOTION

हिन्दी

In general, what are the permissible types of motion for a rigid body that is NOT pivoted or fixed in some way?

  1. It can undergo only pure rotational motion about its geometric centre.
  2. It must undergo pure translational motion without any rotational component.
  3. It can undergo only precession about an arbitrary vertical axis.
  4. It can undergo either pure translation or a combination of translation and rotation.

Correct answer · Option 4

It can undergo either pure translation or a combination of translation and rotation.

Explanation

As stated in the text, the motion of a rigid body which is not pivoted or fixed in some way is either pure translation or a combination of translation and rotation.

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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