Whirling stone in vertical circle.

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Homework Help Overview

The problem involves a stone attached to an inelastic string that is whirling in a vertical circle with a radius of 1.0 m. The tension in the string at the bottom of the circle is stated to be four times that at the top, and the objective is to find the velocity of the stone at the top of the circle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of forces at the top and bottom of the circle, with one suggesting the use of conservation of energy as a potentially simpler method. There are also corrections regarding the angle used in the calculations.

Discussion Status

The discussion includes various perspectives on the solution approach, with some participants affirming the correctness of the original poster's reasoning while others suggest alternative methods. There is no explicit consensus, but the dialogue appears to be productive in exploring different aspects of the problem.

Contextual Notes

Participants note that the original poster was required to solve the problem using forces, which may limit the methods considered. There is also mention of the non-uniform nature of the circular motion, prompting questions about the applicability of conservation of energy.

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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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