A sphere of radius 'R' is rolling with angular velocity 'w'. Find 'w' so that it can just climb the step of height 'h'.
The law of conservation of energy:
T + U = const T + U = \text{const} T + U = const T T T - kinetic energy
T = m v 2 2 + l w 2 2 T = \frac{m v^{2}}{2} + \frac{l w^{2}}{2} T = 2 m v 2 + 2 l w 2
where:
- m - mass of the body
- v - speed of center mass
- l l l - moment of inertia (for sphere equals 2 3 m R 2 \frac{2}{3} m R^2 3 2 m R 2 )
- w w w - angular velocity
If it rolling = w R = wR = wR , therefore
T = 1 2 m w 2 R 2 + 1 3 m w 2 R 2 = 5 6 m w 2 R 2 T = \frac{1}{2} m w^{2} R^{2} + \frac{1}{3} m w^{2} R^{2} = \frac{5}{6} m w^{2} R^{2} T = 2 1 m w 2 R 2 + 3 1 m w 2 R 2 = 6 5 m w 2 R 2 U = m g h U = mgh U = m g h - potential energy
where:
- g - gravitational acceleration
- h - high
T 1 + U 1 = T 2 + U 2 T_{1} + U_{1} = T_{2} + U_{2} T 1 + U 1 = T 2 + U 2
- 1 - initial state
- 2 - final state
U 1 = 0 , T 2 = 0 : U_{1} = 0, T_{2} = 0: U 1 = 0 , T 2 = 0 : T 1 = U 2 T_{1} = U_{2} T 1 = U 2
Therefore:
5 6 m w 2 R 2 = m g h \frac{5}{6} m w^{2} R^{2} = m g h 6 5 m w 2 R 2 = m g h
Finally:
w = 6 g h 5 R 2 w = \sqrt{\frac{6 g h}{5 R^{2}}} w = 5 R 2 6 g h
Answer: w = 6 g h 5 R 2 w = \sqrt{\frac{6 g h}{5 R^{2}}} w = 5 R 2 6 g h