The relationship between the kinetic energy (\( K \)), moment of inertia (\( I \)), and angular velocity (\( \omega \)) is given by:
\[K = \frac{1}{2} I \omega^2\]Now, considering the ratio of the kinetic energies of a sphere and a cylinder, we can write:
\[\frac{ K_{\text{sphere}}}{K_{\text{cylinder}}} = \frac{I_{\text{sphere}}}{I_{\text{cylinder}}} \left( \frac{\omega_{\text{sphere}}}{\omega_{\text{cylinder}}} \right)^2\]Substitute the moments of inertia for a solid sphere and a solid cylinder. The moment of inertia of a solid sphere is:
\[I_{\text{sphere}} = \frac{2}{5} M R^2\]And the moment of inertia of a solid cylinder is:
\[I_{\text{cylinder}} = \frac{1}{2} M R^2\]Now substitute these into the energy ratio equation:
\[\frac{ K_{\text{sphere}}}{K_{\text{cylinder}}} = \frac{\frac{2}{5} M R^2}{\frac{1}{2} M R^2} \left( \frac{\omega}{2 \omega} \right)^2\]Simplifying the equation, we get:
\[= \frac{\frac{2}{5}}{\frac{1}{2}} \left( \frac{1}{2} \right)^2\]Now, simplify the fractions and powers:
\[= \frac{2}{5} \times \frac{2}{1} \times \frac{1}{4}\]Finally, multiplying the terms gives:
\[= \frac{4}{5} \times \frac{1}{4} = \frac{1}{5}\]Thus, the ratio of the kinetic energies is:
\[1 : 5\]This means that the kinetic energy of the sphere is \( 1/5 \)th of that of the cylinder under the given conditions.
Given:
- A solid sphere of mass $m$ and radius $R$ rotating about its diameter with angular speed $\omega$
- A solid cylinder of same mass and radius rotating about its axis with angular speed $2\omega$
Rotational Kinetic Energy formula:
\(E = \frac{1}{2} I \omega^2\)
Moment of Inertia (I):
- For solid sphere about diameter:
\(I_{\text{sphere}} = \frac{2}{5} m R^2\)
- For solid cylinder about its axis:
\(I_{\text{cylinder}} = \frac{1}{2} m R^2\)
Step 1: Rotational KE of sphere
\(E_{\text{sphere}} = \frac{1}{2} \cdot \frac{2}{5} m R^2 \cdot \omega^2 = \frac{1}{5} m R^2 \omega^2\)
Step 2: Rotational KE of cylinder
Angular speed is $2\omega$, so:
\(E_{\text{cylinder}} = \frac{1}{2} \cdot \frac{1}{2} m R^2 \cdot (2\omega)^2 = \frac{1}{4} m R^2 \cdot 4\omega^2 = m R^2 \omega^2\)
Step 3: Ratio of kinetic energies
\(\frac{E_{\text{sphere}}}{E_{\text{cylinder}}} = \frac{\frac{1}{5} m R^2 \omega^2}{m R^2 \omega^2} = \frac{1}{5}\)
Final Answer:
\(\boxed{1:5}\)
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
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 :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :