Forest UCM NLM Oscilations
Skate boarder in Half pipe
Consider a frictionless skateboard released from the top of a semi-circle (half pipe) and oriented to fall directly towards the bottom. The semi-circle has a radius
and the skateboard has a mass .Note: because the skateboard is frictionless, its wheels are not going to turn.
Step 1: System
The skateboard of mass
is the system.Step 1: Coordinate system
Polar coordinate may be a good coordinate system to use since the skateboard's motion will be along the half circle.
Step 3: Free Body Diagram
Step 4: External Force vectors
Step 5: apply Netwon's 2nd Law
For the case of circular motion at constant
The r-hat direction
- centripetal acceleration
The phi-hat direction
- small angle approximation
If we release the skateboard close to the bottom
Then
This approximation make the differential equation easier to solve as it looks more like the simple harmonic motion typical of a spring.
where
- oscillation frequency
The general solution for this second order differential equation may be written as