To solve the problem, we need to find the speed of a solid sphere rolling without slipping down an inclined plane of height 3 m.
1. Given Data:
Mass of sphere, $m = 2\, kg$
Radius of sphere, $r = 0.5\, m$
Height of incline, $h = 3\, m$
Acceleration due to gravity, $g = 9.8\, m/s^2$
2. Using Energy Conservation Principle:
Potential energy at top = Kinetic energy at bottom (translational + rotational)
$ mgh = \frac{1}{2} mv^2 + \frac{1}{2} I \omega^2 $
3. Moment of Inertia and Rolling Condition:
For a solid sphere, $I = \frac{2}{5} mr^2$
Rolling without slipping: $v = \omega r \Rightarrow \omega = \frac{v}{r}$
4. Substitute and Simplify:
$ mgh = \frac{1}{2} mv^2 + \frac{1}{2} \times \frac{2}{5} mr^2 \times \left(\frac{v}{r}\right)^2 $
$ mgh = \frac{1}{2} mv^2 + \frac{1}{5} mv^2 $
$ mgh = \left(\frac{1}{2} + \frac{1}{5}\right) mv^2 = \frac{7}{10} mv^2 $
5. Solve for $v$:
$ gh = \frac{7}{10} v^2 \Rightarrow v^2 = \frac{10}{7} gh $
$ v = \sqrt{\frac{10}{7} \times 9.8 \times 3} $
6. Calculate Numerical Value:
$ v = \sqrt{\frac{10}{7} \times 29.4} = \sqrt{42} = 6.48\, m/s $
Final Answer:
The speed of the sphere at the bottom is $ {6.48\, m/s} $.
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.