To solve the problem of finding the moment of inertia of a ring formed from a rod, we start with understanding the distribution of mass and geometry:
Thus, the moment of inertia of the ring about any of its diameters is \(\frac{\lambda L^3}{8\pi^2}\), which corresponds to the correct answer.
For a rod of length \( L \) and linear mass density \( \lambda \),
the total mass \( m \) of the rod is: \( m = \lambda L \)
When the rod is bent into a ring of radius \( R \), the mass is uniformly distributed along the circumference of the ring.
The moment of inertia of the ring about any of its diameters is given by the formula for a ring: \( I = \frac{1}{2} m R^2 \)
Substituting
\( m = \lambda L \) into this expression: \( I = \frac{1}{2} \lambda L R^2 \)
We know that the circumference of the ring is \( 2\pi R \), and the length of the rod is equal to the circumference of the ring, so: \( L = 2\pi R \)
Thus, the radius \( R \) can be written as: \( R = \frac{L}{2\pi} \)
Substituting this into the equation for the moment of inertia: \( I = \frac{1}{2} \lambda L \left( \frac{L}{2\pi} \right)^2 = \frac{1}{2} \lambda L \times \frac{L^2}{4\pi^2} \)
Simplifying:
\( I = \frac{\lambda L^3}{8\pi^2} \)
Thus, the moment of inertia of the ring about any of its diameters is \( \frac{\lambda L^3}{8\pi^2} \).
Therefore, the correct answer is Option (1).
A wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg m².
Let a line passing through the point $ (4,1,0) $ intersect the line $ L_1: \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} $ at the point $ A(\alpha, \beta, \gamma) $ and the line $ L_2: x - 6 = y = -z + 4 $ at the point $ B(a, b, c) $. Then $ \begin{vmatrix} 1 & 0 & 1 \\ \alpha & \beta & \gamma \\ a & b & c \end{vmatrix} \text{ is equal to} $