Difference in tension introduced by friction

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Homework Help Overview

The discussion revolves around understanding the difference in tension introduced by friction in a scenario involving a cord interacting with a pole. The problem touches on concepts of normal force, centripetal force, and friction in the context of physics, particularly in mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between normal force and tension, questioning the validity of formulas presented. There are discussions about the assumptions made regarding the mass of the cord and the implications for the forces acting on the cord as it interacts with the pole.

Discussion Status

There is an ongoing exploration of different interpretations of the forces at play, with some participants suggesting simplifications to aid understanding. Guidance has been offered regarding the calculation of normal force and the role of small angle approximations, but no consensus has been reached on the correct approach to the problem.

Contextual Notes

Participants note the lack of specific information regarding the mass or density of the cord, which complicates the analysis. The discussion also highlights the importance of understanding the units involved in the equations presented.

Ithilrandir
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Homework Statement
A cord moving at a low speed v rubs against a round post and deviates from a straight line by a small angle Δθ << 1 radian, as shown in the figure. If the tension on one side of the post is T + ΔT and on the other side is T, what is the difference ΔT introduced by the friction?
Relevant Equations
...
I have no clue how to do this, so I did my best guess of it.

Friction is μN, N being the normal force.

The normal force when it is in contract with the pole should be V2/R, R being the radius of the pole.

So ΔT = μV2/R

The answer provided is μTΔθ
 

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Ithilrandir said:
The normal force when it is in contract with the pole should be V2/R, R being the radius of the pole.
In a typical exercise involving cords, pulleys and the like, the cord is approximated as having negligible mass.

There is a different way to determine the normal force based on the givens of the problem together with the assumption that the cord has negligible mass.

There is also a problem with the formula: ##F=\frac{v^2}{r}##. What are the units on the left. What are the units on the right?
 
jbriggs444 said:
In a typical exercise involving cords, pulleys and the like, the cord is approximated as having negligible mass.

There is a different way to determine the normal force based on the givens of the problem together with the assumption that the cord has negligible mass.

There is also a problem with the formula: ##F=\frac{v^2}{r}##. What are the units on the left. What are the units on the right?
I can't see anything wrong with the formula as the force experienced by the cord is by turning a small degree against the post.
 
Ithilrandir said:
I can't see anything wrong with the formula as the force experienced by the cord is by turning a small degree against the post.
Again, answer the question: What are the units on the left? What are the units on the right?

Or, perhaps more obviously: What is the correct formula for centripetal force?

Additionally:

In what direction does a hypothetical centripetal force act on a segment of string?
In what direction does the normal force from the cylinder act on the segment of string?
Do you see that your formula has the wrong sign?!
The faster a [massive] cord moves around this cylinder, the smaller the normal force must become. Which is why an assumption that the cord is massless is so very handy.
 
Last edited:
Ithilrandir said:
I can't see anything wrong with the formula as the force experienced by the cord is by turning a small degree against the post.
Centripetal force has almost nothing to do with the force between the cord and the post.
True, there will be some centripetal force required to coax the cord around the post, but it would be very small and anyway we are not given any mass or density for the cord so it is unknowable.
What centripetal force there is is provided by the tension in the cord, thereby slightly reducing the normal force.
So a) your equation for centripetal force is wrong because the expression on the right is not a force;
b) centripetal force is irrelevant to the question anyway.

Consider the short segment of cord in contact with the post. What are the forces on it?
 
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haruspex said:
Centripetal force has almost nothing to do with the force between the cord and the post.
True, there will be some centripetal force required to coax the cord around the post, but it would be very small and anyway we are not given any mass or density for the cord so it is unknowable.
What centripetal force there is is provided by the tension in the cord, thereby slightly reducing the normal force.
So a) your equation for centripetal force is wrong because the expression on the right is not a force;
b) centripetal force is irrelevant to the question anyway.

Consider the short segment of cord in contact with the post. What are the forces on it?
Right I see. The forces on the segment should be the friction, the normal force and the tension from both sides.
 
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Ithilrandir said:
Right I see. The forces on the segment should be the friction, the normal force and the tension from both sides.
OK I did a force body diagram, with T to the right, F to the left, N upwards and T + ΔT at an angle Δθ to the horizontal.

Using small angle approximation,

(T + ΔT)Δθ = N,

μ(T + ΔT)Δθ = F

(T + ΔT)cosΔθ = T - F, small angle approx,

T + ΔT = T - F

ΔT = F

μ(T + ΔT)Δθ = ΔT

If the μΔTΔθ part of the above is gone I would have the correct answer, but I don't see how to do it from here.
 
Ithilrandir said:
(T + ΔT)Δθ = N
I think that you are letting the ##\Delta T## distract you here. Take one step at a time. You are trying to first compute the normal force ##N##. Then you can use that to figure out ##\Delta T##.

Since ##\Delta T## is small relative to ##T##, one can simplify this to ##N = T \Delta \theta##. This is a simpler and less distracting starting point.
 
jbriggs444 said:
I think that you are letting the ##\Delta T## distract you here. Take one step at a time. You are trying to first compute the normal force ##N##. Then you can use that to figure out ##\Delta T##.

Since ##\Delta T## is small relative to ##T##, one can simplify this to ##N = T \Delta \theta##. This is a simpler and less distracting starting point.
Right. Thanks, I tend to overlook simplifying things involving small values unless it's an angle.
 

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