Moment of inertia of a disc of mass \(M\) and radius \(R\) about any of its diameters is \(\frac{MR^2}{4}\). The moment of inertia of this disc about an axis normal to the disc and passing through a point on its edge will be, \(\frac{x}{2}MR^2\). The value of \(x\) is _________.
Remember the perpendicular and parallel axis theorems. They are essential for calculating moments of inertia about different axes.
The moment of inertia (I) of a disc about any of its diameters is given by \(I_d = \frac{MR^2}{4}\). Using the perpendicular axis theorem, the moment of inertia about an axis perpendicular to the disc and passing through its center is:
\(I_{center} = I_x + I_y = 2 \cdot I_d = 2 \cdot \frac{MR^2}{4} = \frac{MR^2}{2}\)
For the moment of inertia about an axis normal to the disc and passing through a point on its edge, we apply the parallel axis theorem:
\(I_{edge} = I_{center} + Md^2\), where \(d = R\) (the distance from the center to the edge).
So, \(I_{edge} = \frac{MR^2}{2} + MR^2 = \frac{3MR^2}{2}\).
According to the problem, \(I_{edge} = \frac{x}{2}MR^2\). Equating the two expressions for \(I_{edge}\), we get:
\(\frac{x}{2}MR^2 = \frac{3MR^2}{2}\).
Solving for \(x\), we find \(x = 3\).
This value of \(x\) falls within the expected range of 3,3.
A circular disc has radius \( R_1 \) and thickness \( T_1 \). Another circular disc made of the same material has radius \( R_2 \) and thickness \( T_2 \). If the moments of inertia of both the discs are same and \[ \frac{R_1}{R_2} = 2, \quad \text{then} \quad \frac{T_1}{T_2} = \frac{1}{\alpha}. \] The value of \( \alpha \) is __________.
A solid cylinder of radius $\dfrac{R}{3}$ and length $\dfrac{L}{2}$ is removed along the central axis. Find ratio of initial moment of inertia and moment of inertia of removed cylinder. 