Difference between revisions of "Forest UCM NLM Oscilations"
		
		
		
		
		
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| Line 20: | Line 20: | ||
| ==Step 4: External Force vectors== | ==Step 4: External Force vectors== | ||
| + | |||
| + | :<math>\vec{F}_g = -mg \cos \theta \hat{r} - mg \sin \theta \hat{\phi}</math> | ||
| + | :<math>\vec{N} = N \hat{r}</math> | ||
| ==Step 5: apply Netwon's 2nd Law== | ==Step 5: apply Netwon's 2nd Law== | ||
| [[Forest_UCM_NLM#Oscillatiions]] | [[Forest_UCM_NLM#Oscillatiions]] | ||
Revision as of 12:04, 31 August 2014
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.