Circular Motion/Energy: Find the position of the rings when tension = 0

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Homework Help Overview

The discussion revolves around a problem in circular motion and energy, specifically focusing on determining the position of rings in a system when the tension is zero. Participants are analyzing the forces acting on the rings and the conditions under which tension ceases to exist.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss calculations related to the speed of the rings and the forces acting on them, including the normal force and centripetal force. Questions are raised about the validity of certain equations and their application to the scenario, particularly regarding the definition of the angle theta and its implications for tension.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the equations and the physical setup. Some guidance has been offered regarding checking special cases of the angle, and there is an acknowledgment of the need to clarify the definitions used in the problem.

Contextual Notes

Participants are working under the constraints of a homework problem, which may limit the information available for resolving the issues discussed. There is a focus on balancing forces and the implications of mechanical energy conservation in the context of the problem.

Edidas
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Homework Statement
A smooth circular track of mass m is vertically hung by a string down the ceiling. Two small rings, each of mass 3m are initially at rest at the top of the track. They then slide down simultaneously along the track in opposite directions. Find the position of the rings when the tension in the string is zero.
Relevant Equations
Conservation of Energy
mgh = 1/2mv^2
Centripetal Force
Fc = mv^2/r
Here's my first attempt at a solution:

First, I calculated the speed of one ring at the point where the tension would be zero.
3mgr(1-cosΘ ) = (1/2) * (3m) * (v^2).
3m * v^2 = 6mgr(1-cosΘ)

Next, since I wanted the centripetal force, I took the result I got and divided by the radius.
Fc = 6mg(1-cosΘ)

Since I wanted to balance the forces, I calculated the normal force of the hoop on one of the rings.
N - (3mg * cosΘ) = Fc
N = 3mg * (2 - cosΘ)

Then to balance the vertical, I needed the vertical component of the normal force to be equal to the weight of the large hoop. Since there were two rings, I multiplied my initial result by 2.
2 * N * cosΘ = mg.

Simplifying, I got:
6 cos^2(Θ) - 12 cos (Θ) + 1 = 0

The correct answer was Θ = 73° and I do not understand where my error is. I do suspect that it may be in my normal force calculation or the balancing of the vertical forces.

Thanks.
 

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Edidas said:
N - (3mg * cosΘ) = Fc
Check that by considering special cases of the angle.
 
Edidas said:
First, I calculated the speed of one ring at the point where the tension would be zero.
3mgr(1-cosΘ ) = (1/2) * (3m) * (v^2).
3m * v^2 = 6mgr(1-cosΘ)
Why does this equation give the point where the tension is zero? It looks like the mechanical energy conservation equation that applies to all points.
 
Last edited:
kuruman said:
Why does this equation give the point where the tension is zero? It looks like the mechanical energy conservation equation that applies to all points.
That bothered me until I realized @Edidas had mentally defined the angle theta to be that point. Of course , the equation is true for all theta.
 
haruspex said:
Check that by considering special cases of the angle.
I looked at when Θ = 0° and determined that N = 3mg so in that case would it be N + 3mgcosΘ = Fc?
 
haruspex said:
That bothered me until I realized @Edidas had mentally defined the angle theta to be that point. Of course , the equation is true for all theta.
So ##\theta## and ##v## are their respective "critical" values such that the tension is zero. This is appears backwards to me, but OK.
 

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