The Physics Behind Why a Rope Breaks When Falling from a Cliff

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    Falling Physics Rope
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Discussion Overview

The discussion centers on the physics of why a rope can break when a climber falls from a height while attached to it, contrasting the forces involved when a climber is simply hanging from the rope. Participants explore the implications of momentum, force, and the properties of different types of climbing ropes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that the increased momentum from a fall leads to greater forces exerted on the rope than when a climber is simply hanging.
  • One participant notes that climbing ropes are designed to withstand falls to a certain extent, implying that breaking is not guaranteed.
  • There is a discussion about the average force exerted on the rope during a fall, with calculations involving deceleration and the force of gravity.
  • Another participant highlights the importance of rope stretch, noting that climbing ropes are made of materials like nylon that allow for some elasticity to absorb shock.
  • One participant raises concerns about the dangers of using non-stretchy ropes, citing historical engineering failures due to rigidity.
  • Discussion includes the concept of fall factors and how the length of the fall affects the dynamics of the rope's stretch and the forces involved.
  • Some participants mention the energy absorbed by the rope and how it relates to the potential for injury during a fall.

Areas of Agreement / Disagreement

Participants express differing views on the likelihood of a rope breaking during a fall, with some arguing that ropes are designed to handle falls while others emphasize the risks involved. The discussion remains unresolved regarding the exact mechanics and implications of rope failure under different conditions.

Contextual Notes

Participants mention various assumptions regarding the properties of ropes, the nature of falls, and the calculations involved in determining forces and energy transfer. There is also mention of the limitations of certain types of ropes and their ratings.

Who May Find This Useful

This discussion may be of interest to climbers, engineers, and physics enthusiasts who are curious about the mechanics of climbing safety and the physics of forces involved in falls.

Dacourt
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Hi
In a school interview the physics teacher me why a rope attached to the top of a cliff, which would support a climber's weight while dangling gently, would break if the same climber fell from a height while attached to the rope.
Im guessing it's due to increased momentum but the rope equations and ratings I've seen don't really reflect that. It's also the kind of thing it's hard to Google. I've even asked a physicist (medical). It's probably quite simple but has been on my mind for 32 years! Any input appreciated.
 
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Rope equations?
 
Dacourt said:
why a rope attached to the top of a cliff, which would support a climber's weight while dangling gently, would break if the same climber fell from a height while attached to the rope.
For the rope to bring the falling climber to rest in a short distance (the rope cannot stretch that much) it must exert a much greater force on the climber than just his weight. If that force exceeds the breaking strength of the rope -- oops! Climbing ropes are rated for being able to withstand such falls.
 
I think "would break" is a little dramatic; I rather suspect climbing ropes are designed to cope with a fall from height, up to a point, not just a dangling climber.
However, to answer the question. What force is exerted on the rope by a dangling climber of mass m? Suppose he falls from height and is falling at velocity 10 m/s when the rope arrests him. What is the momentum transferred to the rope? If his velocity drops from 10 to 0 over, say, 0.1 s, what is the (average) force exerted on the rope during this time? See where this is going?
 
So
mjc123 said:
I think "would break" is a little dramatic; I rather suspect climbing ropes are designed to cope with a fall from height, up to a point, not just a dangling climber.
However, to answer the question. What force is exerted on the rope by a dangling climber of mass m? Suppose he falls from height and is falling at velocity 10 m/s when the rope arrests him. What is the momentum transferred to the rope? If his velocity drops from 10 to 0 over, say, 0.1 s, what is the (average) force exerted on the rope during this time? See where this is going?
So it's F=ma where a is deceleration and the force on the rope is greater than just dangling?
 
Dacourt said:
So it's F=ma where a is deceleration ...
... plus 1g, if F is the total rope force. Otherwise F is the difference to just hanging still.
 
A.T. said:
... plus 1g, if F is the total rope force. Otherwise F is the difference to just hanging still.
That makes sense. Thank you!
 
Doc Al said:
the rope cannot stretch that much
Not as much as a bungy! but simple climbing ropes are made of nylon (or similar) which is very stretchy, for that purpose - to spread the impulse force over a relatively long time. A polyester rope would snap a falling climber in half as it has a much higher modulus.
This link suggests that the maximum G that a human can survive with a fall is 15g. It isn't clear what evidence that figure is based on but it could be something to work with and suggests that's the extreme value that your rope should be subjecting you to. Assume the climber falls with a rope that's just within its strength limit.
If you equate the kinetic energy gained from a fall of h (mgh) to the energy stored in the (ideal hooke's law) stretched rope (kx2/2) where k is the modulus and x is the amount of stretch or Fx/2 where F is the maximum force. Acceleration is ma and acceleration is 15G so
x/h=2g/a, giving a/h (fractional extension) will be about 1/7. That seems a lot to me but the basic calculation seems to check out. The only thing I left out is the energy absorbed by (friction within) the rope. That would reduce the 1/7 figure by quite a bit, perhaps.
A heavier duty rope would not stretch as much - and kill the climber with excess G and a lighter rope would snap and the climber would die.
In practice, I believe they use harnesses with friction coupling and a higher modulus rope. The coupling provides the friction.
 
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  • #10
sophiecentaur said:
Not as much as a bungy! but simple climbing ropes are made of nylon (or similar) which is very stretchy, for that purpose - to spread the impulse force over a relatively long time. A polyester rope would snap a falling climber in half as it has a much higher modulus.
Good point!
 
  • #11
I suspect that any rope that has little or no stretchyness would be more likely to break since the distance over which the rope must arrest the fall is much less, meaning more force per distance of stoppage.

My father who was an aeronautical engineer who worked on the Lockheed Electra during its crisis in the late '50's had this same problem. The wings and engine mounting assemblies were so rigid that the natural wing flutter and engine vibrations tore the airplane apart. There was no give.

tex
 
  • #12
One thing that probably needs to be pointed out is, rope has a certain stretch *per unit length*. That actually means, by the very nature of the activity, the higher from where you fall, the more rope you fall on, which in turn means it gives more. So, long falls don't necessarily mean more injury than short ones, provided the rope catches you.

That said, dynamic rope has a certain number of "factor-2 falls" ( https://en.m.wikipedia.org/wiki/Fall_factor ) after which the manufacturer suggests retiring it.
 
  • #13
rumborak said:
One thing that probably needs to be pointed out is, rope has a certain stretch *per unit length*. That actually means, by the very nature of the activity, the higher from where you fall, the more rope you fall on, which in turn means it gives more. So, long falls don't necessarily mean more injury than short ones, provided the rope catches you.

That said, dynamic rope has a certain number of "factor-2 falls" ( https://en.m.wikipedia.org/wiki/Fall_factor ) after which the manufacturer suggests retiring it.
The length of rope can be a lot greater than the fall distance it it passes over the top 'eye' and back down again (all the rope can stretch). This is all good news to the guy on the way down.
Of course, the simple mathematical statement about the peak G being independent of the length of the fall, is right as far as it goes. However, the longer the fall, the longer the time that the victim is actually exposed to high forces (Impulse = Force times time) so I'd rather fall 2m than 20m, however suitable the rope happens to be.
 

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