The moment of inertia \( I \) for a thin rod, about an axis through its midpoint and perpendicular to its length, is defined as:
$$ I = \frac{1}{12} M L^2 $$
Here, \( M \) represents the rod's mass, and \( L \) is its length.
Given values:
Substitute the given values into the equation:
$$ 2400 = \frac{1}{12} \times 400 \times L^2 $$
Multiply both sides by 12 to eliminate the fraction:
$$ 2400 \times 12 = 400 \times L^2 $$
$$ 28800 = 400 \times L^2 $$
Divide both sides by 400 to isolate \( L^2 \):
$$ L^2 = \frac{28800}{400} $$
$$ L^2 = 72 $$
Take the square root of both sides to determine \( L \):
$$ L = \sqrt{72} $$
$$ L \approx 8.5 \text{ cm} $$
Consequently, the rod's length is approximately 8.5 cm.
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:
