The problem asks for the ratio of the moment of inertia of a thin circular disk about two axes: the \(z\)-axis and the \(z'\)-axis. Let's solve this problem using the concept of moment of inertia for a circular disk.
For a thin circular disk of mass \(M\) and radius \(R\), the moment of inertia \(I_z\) about an axis perpendicular to the disk (like the \(z\)-axis through its center) is given by:
\(I_z = \frac{1}{2} M R^2\)
The moment of inertia about the \(z'\)-axis, which is perpendicular to the disk through a point on its edge, can be found using the parallel axis theorem. This theorem states that:
\(I_{z'} = I_{z} + M d^2\)
where \(d\) is the distance from the center of the disk to the new axis. Here, \(d = R\) (radius of the disk). Therefore,
\(I_{z'} = \frac{1}{2} M R^2 + M R^2 = \frac{3}{2} M R^2\)
Finally, the ratio of the moment of inertia about the \(z\) and \(z'\)-axes is:
\(\frac{I_z}{I_{z'}} = \frac{\frac{1}{2} M R^2}{\frac{3}{2} M R^2} = \frac{1}{3}\)
Therefore, the correct option is 1:03.
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 