Potentials which depend on positions of two particles

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Discussion Overview

The discussion revolves around the nature of conservative forces, specifically in the context of springs and systems of particles connected by springs. Participants explore the implications of potential energy in these systems, questioning how it is defined and whether energy conservation holds in various scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the force of a spring is conservative when considering two masses linked by a spring, expressing uncertainty about the properties of conservative forces in this context.
  • Another participant asserts that a force is conservative if it depends only on configuration, explaining that work done by such a force can be expressed as a potential energy function, regardless of whether the endpoints of the spring are fixed.
  • A participant expresses gratitude for the explanation of conservative forces and seeks clarification on the implications of the configuration of the spring on work done.
  • Further clarification is provided that the essential factor is the configuration of the spring, not whether its ends are fixed, as the net work done depends solely on the spring's stretch.
  • A participant poses questions about energy conservation in systems involving springs, specifically asking whether potential energy belongs to the spring, the mass, or the system.
  • Another participant responds that the potential energy belongs to the spring and discusses energy conservation in a system of two free masses linked by a spring, suggesting that energy is conserved for the system as a whole.

Areas of Agreement / Disagreement

Participants generally agree on the nature of conservative forces and the role of configuration in defining potential energy. However, there remains some uncertainty regarding the specifics of energy conservation in systems with multiple masses and springs, as well as the ownership of potential energy.

Contextual Notes

Participants express varying levels of understanding regarding the implications of conservative forces and potential energy in different configurations, indicating that assumptions about the system's constraints may affect their reasoning.

Who May Find This Useful

This discussion may be useful for individuals interested in the principles of mechanics, particularly those exploring the concepts of conservative forces, potential energy, and energy conservation in systems involving springs and multiple masses.

BrunoIdeas
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Hello. I have been asked if it is correct to say that the force of a spring is conservative.

So, for a mass attached to a spring on the roof it's OK.
Now consider two masses linked by a spring. Now the potential will depend on both coordinates. It is now not so clear to me any of the properties of conservative forces.
Closed loop integral = 0 and so forth. Neither the fact rot F = 0 => consrevative

Any comments will be appreciated.
 
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It's conservative because any force that depends only on configuration is always conservative. That's because if the force depends only on configuration, then the work done by that force will always be expressible in terms of a potential energy function, via the line integral of that force over deformations of the configuration. The simplest way to see this, especially for 1D deformations like that of a spring, is to simply reverse the path-- if the force depends only on the 1D deformation, then you can get all the work back just by reversing the path of the deformation. If you can always get the work back, it's conservative. Note this doesn't require that either end of the spring be locked down, the work done on the endpoints depends only on the force and the change in the stretch of the spring, because that change is the difference in work on the two ends (given that the force on the two ends is equal and opposite, as per Newton's third law).
 
Ken G said:
It's conservative because any force that depends only on configuration is always conservative. That's because if the force depends only on configuration, then the work done by that force will always be expressible in terms of a potential energy function, via the line integral of that force over deformations of the configuration. ... then you can get all the work back just by reversing the path of the deformation. If you can always get the work back, it's conservative. Note this doesn't require that either end of the spring be locked down, the work done on the endpoints depends only on the force and the change in the stretch of the spring, because that change is the difference in work on the two ends (given that the force on the two ends is equal and opposite, as per Newton's third law).

I am so grateful for your answer. I particularly apreciate you've given me the intuiton about understanding conservative forces as position dependent and the notion of getting work back. Using this one evidently sees why friction is not, and probably why it conflicts with time invariance or reversal of Newton's eqs.

I however do not fully understand what is after the bold text.

Once again thanks.
 
I think you understand completely, the stuff after the bolded text was in there just because it sounded like you could understand this better if one end of the spring was locked down, but if both ends were free to move around it wasn't so clear. I was trying to show that it doesn't matter if either end is locked down, what matters is that if the configuration of the spring is all you need to know the force it is applying at both ends, then the net work done only depends on the configuration (i.e., the stretch) of the spring, and re-extracting that work is also only dependent on returning to the original configuration, even if the spring has waffled around in the mean time.
 
Fine. Thanks, I get that. Now I would like to ask what about energy conservation in such cases.
1) Consider a mass attached to a spring hooked from the ceiling with no gravity (or with it, it does not matter). We say that energy is conserved because forces are conservative.
Question: Does the potential energy belong to the spring, to the mass, or to the system.

I understand this question may be misleading but answer me as if I knew nothing.


2) Consider the two masses linked by a spring. Is energy conserved? I understand/guess that for the system it it, not for the masses, but I cannot give good arguments. Could you help me?


Thanks Ken G, and everyone.
 
BrunoIdeas said:
Question: Does the potential energy belong to the spring, to the mass, or to the system.
The potential energy belongs to the spring. It is stored in interparticle forces within the spring. If you remove the mass completely, all the potential energy is still in that spring, as anyone has discovered to their chagrin if they did remove the mass suddenly!
2) Consider the two masses linked by a spring. Is energy conserved? I understand/guess that for the system it it, not for the masses, but I cannot give good arguments. Could you help me?
Energy is conserved if there are two free masses linked by a spring. The sum of the kinetic energies of the two masses, plus kx2/2 for the spring, will always be the same. I'm not sure what aspect of this is where your question is focused.
 

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