Whirling stone in vertical circle.

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A stone attached to an inelastic string is analyzed as it whirls in a vertical circle with a radius of 1.0 m. The tension at the bottom of the circle is four times that at the top, leading to equations for the velocities at both positions. The calculations confirm that the velocity at the top can be derived using force equations, though conservation of energy could simplify the process. Corrections in the discussion clarify the angle used in calculations, affirming that the top position corresponds to θ = π. The final conclusion is that the solution appears correct, despite the complexities of non-uniform circular motion.
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Homework Statement


A stone, attached to one end of an inelastic string whirls around in a vertical circle of 1.0 m radius. The tension in the string when the stone is at the bottom of the circle is found to be four times the tension in the string when the stone is at the top. Find the velocity of the stone when it is at the top of the circle.

Homework Equations


ΣF=ma
arad = vt²/r
vt = rω
x-direction right = positive
y-direction up = positive
assuming it spins at counter clockwise direction = positive

The Attempt at a Solution


At the top of the circle:
ΣF=ma
-T-mg = marad = -mvtop²/r
vtop2 = (T+mg)/m

At the bottom of the circle:
ΣF=ma
4T-mg = mvbottom2/r
vbottom2 = (4T-mg)/m

At an angle θ counter clockwise from the vertical axis:
-mgsinθ = mat
-gsinθ = dVt/dθ x dθ/dt
∫ -rgsinθ dθ = ∫ Vt dVt
rgcosθ = 0.5Vt2 + c

When θ = 0, and r =1.0, Vt2 = vbottom2 = (4T-mg)/m
c = g - (4T-mg)/2m
Therefore, Vt2 = (4T-mg)/m + 2gcosθ - 2g

When θ = 2π, Vt2 = vtop2 = (T+mg)/m
(4T-mg)/m - 4g = (T+mg)/m
T= 2mg

vtop2 = (T+mg)/m = 3g

vtop = -(3g)Is my answer correct?
 
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seems correct to me, though it would ve been a bit more simple if you had use conservation of energy for the top and bottom position.

Small corection (doesnt affect the final result since it seems you used cos(2pi)=-1), for the top position it is \theta=\pi not \theta=2\pi
 
Last edited:
Yoonique said:
A stone, attached to one end of an inelastic string whirls around in a vertical circle of 1.0 m radius. The tension in the string when the stone is at the bottom of the circle is found to be four times the tension in the string when the stone is at the top. Find the velocity of the stone when it is at the top of the circle.
Is that an exact reproduction of the problem statement?
 
Delta² said:
seems correct to me, though it would ve been a bit more simple if you had use conservation of energy for the top and bottom position.

Small corection (doesnt affect the final result since it seems you used cos(2pi)=-1), for the top position it is \theta=\pi not \theta=2\pi

Thanks, noted my mistake. I was required to do it by forces though.
 
AlephNumbers said:
Is that an exact reproduction of the problem statement?
Yes it is the exact question.
 
Then I think your solution is correct.
 
Delta² said:
seems correct to me, though it would ve been a bit more simple if you had use conservation of energy for the top and bottom position.

Small corection (doesnt affect the final result since it seems you used cos(2pi)=-1), for the top position it is \theta=\pi not \theta=2\pi
How could you use conservation of energy if the circular motion is not uniform?
 
Well the work of the tension is zero ( string is inelastic, tension is always perpendicular to velocity), we have only work of the weight involved which is a conservative force so conservation of energy applies.
 
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