Potential Energy for "stone + field" physical system

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Discussion Overview

The discussion revolves around the concept of potential energy in the context of a stone falling in the Earth's gravitational field. Participants explore different models of potential energy, considering both classical mechanics and general relativity (GR), and whether potential energy should be attributed to the stone, the field, or the system as a whole.

Discussion Character

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

Main Points Raised

  • Some participants propose that potential energy can be attributed to the field itself when considering the system as "stone + field," suggesting a different perspective from the traditional view of potential energy being associated solely with the stone.
  • Others argue that in general relativity, the concept of potential energy disappears, with energy being measured locally by observers and dependent on the motion of particles through spacetime.
  • A participant questions the meaning of "classically," suggesting that potential energy is often attributed to systems rather than individual particles, as seen in quantum mechanics and classical electrodynamics.
  • Some contributions highlight that many introductory textbooks treat potential energy as a property of the Earth-stone system, emphasizing the need for consistency across different physical theories.
  • There is discussion about the implications of special relativity (SR) on the concept of fields and potential energy, with some suggesting that the concept can still be applied similarly to classical physics.
  • Participants express uncertainty about the adequacy of the "stone in an external assigned field" model, suggesting it may be overly simplistic from an energy perspective.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the attribution of potential energy or the adequacy of different models. Multiple competing views remain regarding the role of potential energy in classical mechanics, general relativity, and special relativity.

Contextual Notes

Limitations include the dependence on definitions of potential energy and the varying interpretations of classical versus modern physics frameworks. The discussion also reflects unresolved questions about the reconciliation of Newtonian gravity with special relativity.

Who May Find This Useful

This discussion may be of interest to students and educators in physics, particularly those exploring the concepts of potential energy, gravitational fields, and the implications of different physical theories.

cianfa72
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Consider the classical scenario a stone falling in the Earth gravitational field.
Classically we attach a Potential Energy to the stone and using the law of conservation of (mechanical) energy we are able to evaluate the dynamic of the falling stone.

This model assume a stone in a "external" field (due to the Earth) with potential energy attached to the stone itself (here the physical system to take in account is actually "the stone").

On the other hand I was thinking we can attach a Potential energy to the field itself considering as physical system the union "stone + field": this way potential energy of the system is basically the energy attached to the field while the kinetic one is that of the stone.

Does it make sense ?
 
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cianfa72 said:
Consider the classical scenario a stone falling in the Earth gravitational field.
Classically we attach a Potential Energy to the stone and using the law of conservation of (mechanical) energy we are able to evaluate the dynamic of the falling stone.

This model assume a stone in a "external" field (due to the Earth) with potential energy attached to the stone itself (here the physical system to take in account is actually "the stone").

On the other hand I was thinking we can attach a Potential energy to the field itself considering as physical system the union "stone + field": this way potential energy of the system is basically the energy attached to the field while the kinetic one is that of the stone.

Does it make sense ?

It's a good question.

If you move to the theory of GR, then the potential energy as a concept disappears (as does the concept of force), except in Newtonian approximations. What you have in GR is the concept of the energy of a particle measured locally (by a local observer). This energy is the kinetic energy (plus the rest-mass energy). The particle has no potential energy, as such. Instead, the different measurements of energy depend on the motion of the particle and the observer through spacetime. (Technically, these are four-velocity of the particle and observer.)

If you take a step further and consider an expanding universe, then you lose the principle of energy conservation. Or, if you want to retain energy conservation, then some energy has to be stored in the gravitational field. There's a good piece about that by Sean Carroll here.

http://www.preposterousuniverse.com/blog/2010/02/22/energy-is-not-conserved/
 
cianfa72 said:
Consider the classical scenario a stone falling in the Earth gravitational field.
Classically we attach a Potential Energy to the stone and using the law of conservation of (mechanical) energy we are able to evaluate the dynamic of the falling stone.

This model assume a stone in a "external" field (due to the Earth) with potential energy attached to the stone itself (here the physical system to take in account is actually "the stone").
With "Classically" what you mean? Classical mechanics?
E. g. when you study the hydrogen energy levels in QM you don't say "the electron energy levels", exactly because this energy must be ascribed to the whole system "atom". Even in classical electrodynamics you usually don't ascribe potential energy to a single charged particle, but to the system of interacting ones.

--
lightarrow
 
lightarrow said:
With "Classically" what you mean? Classical mechanics?
E. g. when you study the hydrogen energy levels in QM ...

Whatever was meant by "classical", it was not QM!
 
lightarrow said:
With "Classically" what you mean? Classical mechanics?
Sure I mean not QM nor GR
Just to be more clear: at basic (undergrad) level the model above is based on an external (let me say assigned) field described by a Potential function (note "Potential" and not "Potential Energy"...maybe here is the root of my confusion). Where is "stored in a form of energy" the work done against the field when the stone changes position in the external field ? We can assume it is "stored" into the Potential Energy of the stone in the field I guess, and here there exist no way to store it in the field itself (the external field is assigned and cannot change).

In the other scenario that also includes in the model the "source" of gravitational field (the Earth body) the physical system to consider is basically "Earth body + field + stone" and this time we are able to "store" the work done in the field itself (now the field is not "assigned" but reflects the interaction between bodies).
 
Last edited:
cianfa72 said:
Classically we attach a Potential Energy to the stone and using the law of conservation of (mechanical) energy we are able to evaluate the dynamic of the falling stone.

Many authors of introductory textbooks and curricula have taken the approach that the potential energy is a property of the Earth-stone system. And moreover that it must be done this way to develop a concept of energy that is consistent across both Newtonian mechanics and thermodynamics.
 
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Mister T said:
Many authors of introductory textbooks and curricula have taken the approach that the potential energy is a property of the Earth-stone system.
Going further and considering SR preventing us to have infinite interaction speed (bound to the speed of the light) I believe also in the simple "Earth+stone" system we are "forced" to introduce the concept of "field" in order to mediate interactions between bodies. This way Earth actually interacts with field as the stone too. Therefore the physical system to take in account is formed actually by "Earth + field + stone" and we can assign to the current field distribution a (potential) energy density in which we can image "stored" the work done to bring the system in the current configuration.

Coming back to the model "stone in an external assigned field", it surely simplify the model to calculate the stone dynamic but from Energy point of view I believe it is poor, what do you think about ?
 
cianfa72 said:
Coming back to the model "stone in an external assigned field", it surely simplify the model to calculate the stone dynamic but from Energy point of view I believe it is poor, what do you think about ?
Or, maybe, it is better to say in that model the system is actually made of "stone + field" with potential energy a property of that system (basically here "the field" acts let me say as a body or "thing")
 
PeroK said:
If you move to the theory of GR, then the potential energy as a concept disappears (as does the concept of force), except in Newtonian approximations. What you have in GR is the concept of the energy of a particle measured locally (by a local observer). This energy is the kinetic energy (plus the rest-mass energy). The particle has no potential energy, as such.
Could you elaborate more this point ? Thanks
 
  • #10
cianfa72 said:
Could you elaborate more this point ? Thanks

Do you have a specific question?
 
  • #11
PeroK said:
Do you have a specific question?
In the context of SR even with finite interaction speed (basically limited by the speed of the light - c) I believe we can still introduce the concept of "field" including the associated potential energy as in the case of "classic" physics. Consider for instance the system made of 2 electric charges: the work done on them by external forces basically increases the "electrical potential energy" of the system that we can image "stored" in distribution of the electric field itself.

Does it make sense ?
 
  • #12
cianfa72 said:
In the context of SR even with finite interaction speed (basically limited by the speed of the light - c) I believe we can still introduce the concept of "field" including the associated potential energy as in the case of "classic" physics.

Does it make sense ?

There were attempts, I believe, to reconcile Newtonian gravity with SR. But, I don't know much about them, except they didn't succeed.
 
  • #13
PeroK said:
There were attempts, I believe, to reconcile Newtonian gravity with SR. But, I don't know much about them, except they didn't succeed.
ok but in this example we are talking about electrical (or electromagnetic) field in the context of SR neglecting GR (for instance spacetime curvature)
 
  • #14
cianfa72 said:
ok but in this example we are talking about electrical (or electromagnetic) field in the context of SR neglecting GR (for instance spacetime curvature)

I thought we were talking about gravity. Maxwell's theory of EM was/is compatible with SR. For example, you have the four-potential:

https://en.wikipedia.org/wiki/Electromagnetic_four-potential
 

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