Let's say I have a ball attached to a string and I'm spinning it above my head. If it's going fast enough, it doesn't fall. I know there's centripetal acceleration that's causing the ball to stay in a circle but this doesn't have to do with the force of gravity from what I understand. Shouldn't the object still be falling due to the force of gravity?
Answer
We have the ball orbiting at a distance R from the centre of rotation and the string inclined at angle θ with respect to the horizontal.
Two main forces act on the ball: gravity mg (m is the mass of the ball, g the Earth's gravitational acceleration) and Fc, the centripetal force needed to keep the ball spinning at constant rate. Fc is given by:
Fc=mv2R,
where v is the orbital velocity, i.e. the speed of the ball on its circular trajectory.
Trigonometry also tells us that if T is the tension in the string, then:
Tcosθ=Fc.
Similarly, as the ball is not moving in the vertical direction, thus Fup:
Tsinθ=Fup=mg.
From this relation we can infer:
T=mgsinθ.
And so:
mgtanθ=Fc=mv2R.
Or:
tanθ=gRv2.
From this follows that for small tanθ and thus small θ we need large v. But at lower v, θ increases. Also note that θ is invariant to mass m.
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