What is the Correct Integral Setup for Finding Tension in a Rope on a Cone?

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Homework Help Overview

The problem involves determining the tension in a rope that is positioned on a cone. The rope's weight and the geometry of the cone, including its top angle and radius at a given height, are central to the discussion. The original poster expresses a desire to understand the correct integral setup for this scenario, particularly in relation to future test questions.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the geometry of the cone and the implications of the rope's placement, questioning whether the cone is oriented with the apex upwards or tilted. There is also consideration of how the rope's weight contributes to tension and the radial forces involved.

Discussion Status

Some participants have provided insights regarding the need for a diagram to clarify the setup. There is an ongoing exploration of the relationship between the rope's weight and the tension, with suggestions to consider previous results related to tension in circular setups. The original poster is encouraged to articulate their reasoning further.

Contextual Notes

There is mention of the potential complexity introduced by the cone's orientation and the radial components of forces. The original poster is also grappling with how certain factors, like the 2*pi factor, may influence their calculations.

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Homework Statement



I am given the weight (force) of the rope as W. It sits on a cone about halfway down, with the cone's top angle ø. Radius at a given placement is r, and h is our height at a given placement.
I need to find the tension, T, in the rope.

Homework Equations



W=mg
Integral (F * dr) = 0
I am taking r to be along the x axis.
L = sqrt(r^2 + h^2)
X = L*cos(ø)
Y = L*sin(ø)
dX = dø*L*-sin(ø)
dY = dø*L*cos(ø)

The Attempt at a Solution



Expressing my equilibrium as:

T*L*dø*cos(ø)-m*g**dø*L*-sin(ø) = 0

I get: T = W*tan(ø)

This seems over simplified? Or am I over-thinking it? It's around a circle radius r and each element of T summed over the circle would be 2*pi*T but the gravitational force is also summed over 2*pi. Perhaps I skipped over the line integral of this? I am very interested in the correct integral setup of this problem because it looks like a future test question, and I also want to know how my 2*pi factor disappears (if it was ever present?) Any help is appreciated.
 
Last edited:
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You need a diagram.

You are given the "top angle" of the cone - which wording suggests that the cone is oriented with the apex upwards, and the rope is draped over the outside. If the rope is draped anywhere below the apex, then it will be draped over a hyperbola - but nothing dangles.

The mention of circles suggests that the cone is tilted so the central axis is horizontal.
In which case, what is stopping you from using a previous result for tension from being draped over a circle?
 
Simon Bridge said:
You need a diagram.

You are given the "top angle" of the cone - which wording suggests that the cone is oriented with the apex upwards, and the rope is draped over the outside. If the rope is draped anywhere below the apex, then it will be draped over a hyperbola - but nothing dangles.

The mention of circles suggests that the cone is tilted so the central axis is horizontal.
In which case, what is stopping you from using a previous result for tension from being draped over a circle?

I suspect that the rope is in fact a circular ring of rope and the OP is meant to find the tension in the rope that results from it being placed on a cone (apex up). The weight of the rope results in an outward radial force all around the circumference which must be countered by a tension in the rope.
 
Image

Thanks guys, here's the diagram.

I get that the weight contributes to the tension, but it is not the full weight that is equal to the tension, but rather the radial component.
 

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Cool - so walk us through the reasoning that leads to your result.
 
Ok, well I consider the constraint, being the solid cone. Any contribution from gravity must then be in the radial direction, normal to the cone. I am trying to find the tension as a function of the angle, and the tangential component of the angle is definitely in the normal direction.
 

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