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Physics · SYSTEMS OF PARTICLES AND ROTATIONAL MOTION

हिन्दी

An ideal rigid body is best defined as a body in which:

  1. The shape changes continuously when external forces act on it.
  2. The distances between all pairs of particles do not change under any circumstances.
  3. The particles are always moving relative to one another with constant speed.
  4. The centre of mass always remains strictly at rest.

Correct answer · Option 2

The distances between all pairs of particles do not change under any circumstances.

Explanation

By definition, a rigid body is ideally a body with a perfectly definite and unchanging shape, such that the distances between all pairs of particles of the body do not change.

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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