The moment of inertia \( I \) of a thin rod about an axis passing through its midpoint and perpendicular to the rod is given by the formula:
$$ I = \frac{1}{12} M L^2 $$
where \( M \) is the mass of the rod, and \( L \) is the length of the rod.
Given:
Substituting the given values into the formula:
$$ 2400 = \frac{1}{12} \times 400 \times L^2 $$
Multiplying both sides by 12 to remove the fraction:
$$ 2400 \times 12 = 400 \times L^2 $$
$$ 28800 = 400 \times L^2 $$
Dividing both sides by 400 to solve for \( L^2 \):
$$ L^2 = \frac{28800}{400} $$
$$ L^2 = 72 $$
Taking the square root of both sides to solve for \( L \):
$$ L = \sqrt{72} $$
$$ L \approx 8.5 \text{ cm} $$
Thus, the length of the rod is approximately 8.5 cm.
The moment of inertia of a rod is given by:
$I = \frac{1}{12}ML^2$.
Here, $I = 2400 \, g cm^2 = 2400 \times 10^{-7} \, kg m^2$, $M = 400 \, g = 0.4 \, kg$.
Rearrange to find $L$:
$L = \sqrt{\frac{12I}{M}} = \sqrt{\frac{12 \times 2400 \times 10^{-7}}{0.4}} = 8.5 \, cm$.
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. 
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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.