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Question:

The general motion of a rigid body can be considered to be a combination of (i) a motion of its center of mass about an axis, and (ii) its motion about an instantaneous axis passing through the center of mass. These axes need not be stationary. Consider, for example, a thin uniform disc welded (rigidly fixed) horizontally at its rim to a mass less stick, as shown in the figure. When the disc-stick system is rotated about the origin on a horizontal frictionless plane with angular speed ω, the motion at any instant can be taken as a combination of (i) a rotation of the center of mass of the disc about the z-axis, and (ii) a rotation of the disc through an instantaneous vertical axis passing through its center of mass (as is seen from the changed orientation of points P and Q. Both these motions have the same angular speed ω in this case. Now consider two similar systems as shown in the figure: Case (a) the disc with its face vertical and parallel to it x-z plane; Case (b) the disc with its face making an angle of 45° with it x-y plane and its horizontal diameter parallel to x-axis. In both the cases, the disc is welded at point P, and the systems are rotated with constant angular speed ω about the z-axis. Which of the following statements regarding the angular speed about the instantaneous axis (passing through the center of mass) is correct?

It is ω for both the cases.

It is √2ω for both the cases.

It is ω for case (a); and ω√2 for case (b).

It is ω for case (a); and √2ω for case (b).

Solution:

Angular velocity of a body doing rotational motion about any axis located on the body is same as that of angular velocity about its COM. As for both cases, angular velocity about z-axis is ω, thus angular velocity about their centre of mass is also ω for both.