Given:
Step 1: Moment of Inertia of a Single Disc
The moment of inertia of a disc about its central axis is:
\[ I_c = \frac{1}{2} m R^2 \]
Step 2: Moment of Inertia of Six Outer Discs
Each outer disc is at a distance \( r = 2R \) from the central axis. Using the parallel axis theorem:
\[ I = I_c + m r^2 \]
\[ I_{ ext{outer}} = \frac{1}{2} m R^2 + m (2R)^2 \]
\[ I_{ ext{outer}} = \frac{1}{2} m R^2 + 4 m R^2 \]
\[ I_{ ext{outer}} = \frac{1}{2} m R^2 + 4 m R^2 = \frac{9}{2} m R^2 \]
Step 3: Total Moment of Inertia
Since there are 6 outer discs:
\[ I_{ ext{total}} = I_{ ext{central}} + 6 I_{ ext{outer}} \]
\[ I_{ ext{total}} = \frac{1}{2} m R^2 + 6 \times \frac{9}{2} m R^2 \]
\[ I_{ ext{total}} = \frac{1}{2} m R^2 + \frac{54}{2} m R^2 \]
\[ I_{ ext{total}} = \frac{55}{2} m R^2 \]
Answer: The moment of inertia of the system is \( \frac{55}{2} m R^2 \) (Option B).
For a uniform rectangular sheet shown in the figure, the ratio of moments of inertia about the axes perpendicular to the sheet and passing through \( O \) (the center of mass) and \( O' \) (corner point) is: