What force is needed to break a rope?

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Homework Help Overview

The discussion revolves around the forces acting on a rope tied to a tree and the conditions under which it would break. The original poster presents a scenario involving tension forces and queries whether the rope will break under different pulling conditions.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the concept of tension in the rope when pulled against a tree versus a person, questioning whether the force exerted by each scenario affects the breaking point of the rope. There are discussions about Newton's laws and the implications of forces acting on the rope.

Discussion Status

The conversation is ongoing, with participants providing insights into the mechanics of forces and tension. Some participants clarify misunderstandings regarding the application of Newton's laws, while others question the definitions and assumptions made in the original scenario.

Contextual Notes

There is a mention of a specific force needed to break the rope (15 N) and the tension forces being discussed (10 N). The implications of pulling forces from different sources (a tree versus a person) are also under scrutiny.

Lotto
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Homework Statement
I pull a rope tied to a tree with 10 N. The force needed to break a rope is 15 N. Will I break the rope? What if two people pull the rope from opposite ends with forces 10 N and -10 N. Will the rope break now?
Relevant Equations
Newtons third law of motion
I would say that it will not break in both cases, since tension force is 10 N, no matter if I pull it against a tree or a person.

But I am not sure. How is it?
 
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Lotto said:
since tension force is 10 N, no matter if I pull it against a tree or a person.
You are exactly right.
 
Lotto said:
Homework Statement: I pull a rope tied to a tree with 10 N. The force needed to break a rope is 15 N. Will I break the rope? What if two people pull the rope from opposite ends with forces 10 N and -10 N. Will the rope break now?
Relevant Equations: Newtons third law of motion

I would say that it will not break in both cases, since tension force is 10 N, no matter if I pull it against a tree or a person.

But I am not sure. How is it?
Sketch a FBD for each case.

In the first, we have a person acting on the rope to, say, the left of 10 N. On the other end we have the tree in a fixed position. Since ideal ropes transmit force, there is a force of 10 N on this tree, acting to the left. Thus, by Newton's 3rd, it is exerting a force of 10 N on rope, acting to the right. The tension in the rope will be will be 10 N, so it will not break.

In the second case, we have almost the same situation. Note that, if the person on the other end didn't move or exert any force, then the tension in the rope is again 10 N. But the person is now exerting a 10 N force to the right, in addition to the force exerted by them by staying still. So now there is an extra 10 N acting on the rope and thus the tension is 20 N. So the rope breaks.

-Dan
 
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topsquark said:
Note that, if the person on the other end didn't move or exert any force,
Then the rope could not be subject to any force from that person. It would be a massless object subject to a non-zero net force. Which is a contradiction to Newton's second law.

Write down the force balance and you will see that to balance forces on the rope, the other person must be exerting a 10 N force, equal and opposite to the force exerted by us. Those two forces are a "second law pair".

The other person exerts the same force on the rope that the tree exerts on the rope. @Lotto has it right. You have it all wrong.
 
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jbriggs444 said:
"second law pair".
Shouldn’t it be a third law pair?
 
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Frabjous said:
Shouldn’t it be a third law pair?
A third law pair is matching up the force of A directly on B with the force of B directly on A. Yes, the third law states that those must be equal and opposite.

If you have an ideal massless object between A and B (call it R for rope) then you have the force of A on R and the force of B on R. Those are not third law partner forces.

But if you write down Newton's second law: ##\sum F = ma## you get ##F_\text{AR} + F_\text{BR} = m_Ra_R = 0## and you can conclude that ##F_\text{AR} = -F_\text{BR}##. I use the term "second law pair" to refer to the two forces in such a situation.

Admittedly, if you are used to reading "third law partner", the notion of a "second law partner" may be jarring. If so, feel free to ignore the phrase and substitute the second law logic.
 
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jbriggs444 said:
Then the rope could not be subject to any force from that person. It would be a massless object subject to a non-zero net force. Which is a contradiction to Newton's second law.

Write down the force balance and you will see that to balance forces on the rope, the other person must be exerting a 10 N force, equal and opposite to the force exerted by us. Those two forces are a "second law pair".

The other person exerts the same force on the rope that the tree exerts on the rope. @Lotto has it right. You have it all wrong.
The issue, then, is that I'm reading the question wrong. I had taken the person to be adding an extra 10 N on top of the 10 N they needed to remain motionless.

Thanks for the catch!

My apologies to all.

-Dan
 
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Lotto said:
I would say that it will not break in both cases, since tension force is 10 N, no matter if I pull it against a tree or a person.
Right. The person pulls with 10 N of force, the tree pulls back with 10 N of force.
In the other case, a person pulls with 10 N of force and a second person pulls back with 10 N of force.

It makes no difference if it's the tree or the second person that's doing the pulling. You get 10 N of tension in the rope either way.
 
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jbriggs444 said:
A third law pair is matching up the force of A directly on B with the force of B directly on A. Yes, the third law states that those must be equal and opposite.

If you have an ideal massless object between A and B (call it R for rope) then you have the force of A on R and the force of B on R. Those are not third law partner forces.

But if you write down Newton's second law: ##\sum F = ma## you get ##F_\text{AR} + F_\text{BR} = m_Ra_R = 0## and you can conclude that ##F_\text{AR} = -F_\text{BR}##. I use the term "second law pair" to refer to the two forces in such a situation.

Admittedly, if you are used to reading "third law partner", the notion of a "second law partner" may be jarring. If so, feel free to ignore the phrase and substitute the second law logic.
I thought the third law was that a robot must protect its own existence as long as such protection does not conflict with the first or second law. I don’t see what that has to do with this rope problem.
 
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