A uniform solid cylinder with radius \(R\) and length \(L\) has a moment of inertia \(I_1\) about the axis of the cylinder. A concentric solid cylinder of radius \(R' = \frac{R}{2}\) and length \(L' = \frac{L}{2}\) is carved out of the original cylinder. If \(I_2\) is the moment of inertia of the carved-out portion, then \(\frac{I_1}{I_2} =\)
(Both \(I_1\) and \(I_2\) are about the axis of the cylinder.)
The moment of inertia for a uniform solid cylinder about its axis is:
\[ I = \frac{1}{2} m R^2 \]
\[ I_1 = \frac{1}{2} m_1 R^2 \]
The mass of the carved-out portion (\(m_2\)) is proportional to its volume:
\[ m_2 = \rho \cdot \text{Volume} = \rho \cdot \pi \left(\frac{R}{2}\right)^2 \cdot \frac{L}{2} = \frac{\rho \pi R^2 L}{8} \]
Moment of inertia:
\[ I_2 = \frac{1}{2} m_2 \left(\frac{R}{2}\right)^2 = \frac{1}{2} \cdot \frac{\rho \pi R^2 L}{8} \cdot \frac{R^2}{4} = \frac{\rho \pi R^4 L}{64} \]
The mass of the original cylinder (\(m_1\)) is:
\[ m_1 = \rho \cdot \pi R^2 L \]
Moment of inertia of the original cylinder:
\[ I_1 = \frac{1}{2} m_1 R^2 = \frac{1}{2} \cdot \rho \pi R^2 L \cdot R^2 = \frac{\rho \pi R^4 L}{2} \]
The ratio is:
\[ \frac{I_1}{I_2} = \frac{\frac{\rho \pi R^4 L}{2}}{\frac{\rho \pi R^4 L}{64}} = \frac{64}{2} = 32 \]
The correct answer is 32.
I1=2m1R2I2=2m2(R/2)2
I2I1=m24m1=ρ⋅4πR2×2ℓ4⋅ρπR2ℓ⇒I2I1=32
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: