I Does the Principle of Least Action Have a Physical Meaning?

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The discussion centers on the differing opinions regarding the physical meaning of the Principle of Least Action (PLA), with some physicists viewing it as fundamental while others see it as merely a mathematical tool. The lack of consensus appears to stem from varying interpretations of what constitutes "physical meaning." Examples, such as the behavior of photons during refraction, illustrate the debate over whether the PLA is inherently physical or just a mathematical outcome. Some participants argue that the extensive experimental support for PLA suggests it has physical significance, while others maintain that its application can be purely mathematical. Overall, the conversation highlights the complexities and nuances in understanding the role of PLA in physics.
  • #31
crastinus said:
What could the physical meaning of PLA even be?

From a laypersons point of view (which may or may not be useful to the OP), I think the answer is yes. The reason being that PLA describes what nature does and if nature didn't do it, PLA would not be valid. It is a direct description of the goings on in nature hence it has physical meaning.

At the suggestion of someone in this forum I watched all of Feynman's lectures and bought and read the book on QED. It was wonderful! I've really learned something new.

Having read the book it seems one could argue that PLA is not fundamental because QED just explains it better. So it seems to me QED is closer and better at allowing us to understand what nature is doing, such as why a light beam reflects off a mirror the way it does. It still only tells us what nature is doing and not why it is doing it, but why nature does certain things (as has been pointed out to me many times in this forum) is not knowable.

So to me, both PLA and QED have physical meaning. Just my lay opinion for what it's worth.
 
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  • #32
The PLA is a 'principle', not a 'fundamental law' or 'axiom' like Newton's axioms. It is usually equivalent to the equation(s) of motion. Now, in many cases, the equation of motion is not fundamental. Example 1: Newton's equation of motion, force = mass x acceleration. It does not enter Newton's axioms. Example 2: The standard (D'Alembert's) wave equation. It is not suitable to represent Huygens' principle.
Nevertheless, the PLA is at least a most powerful tool. For instance, special-relativistic equations can be written down covariantly (manifest invariantly) in a straightforward manner. More generally, its tight connection with the symmetry of the problem under consideration makes the generalization of equations much more easy.​
 
  • #33
A discussion of "The" Principle of Least Action will get confusing if there is more than one principle of least action. Considering only classical mechanics, what assumptions must hold before "a" principle of least action applies? (One can argue subjectively about whether such assumptions make a principle of least action "fundamental" or "not fundamental", but what the assumptions are should be an objective topic.)

anorlunda said:
That is a distinction without meaning. Use your infinitesimal step as having end points A and B. Prove the PLA for that. Now add a second step B to C. and do likewise, now you have a double step A to C. PLAl applies no matter how big or small the step.

That's plausible in a case when a principle of least action applies over a long time interval. However, are there cases when it doesn't? I'm thinking of a classical analog of a "delayed choice" experiment where we vary the force on a particle as a function of space and time and try to trick it into taking a path that is not a stationary path in the action (or where "action" is undefined). For example: "Ah-hah, you started out going due North, but should have stayed where your were for 3 seconds and then taken a Northeasterly trajectory."
 
  • #34
I wonder if the PLA is equivalent to the principle of determinism in dynamics. Let a particle follow a trajectory. Determinism says that at each instant, the momentum and location of the particle are a direct consequence of the previous momentum and location. The trajectory as a whole may be viewed as a sequence of instants, each of which follows from its immediate predecessor, according to the applicable laws of motion. But the trajectory is also given by the PLA. What is the relationship between the PLA description of a trajectory and the deterministic model? I don't know enough physics to establish this connection, but I once asked an instructor if the equivalence was true and he replied in the affirmative, without elaboration.

As an example of a purely mathematical justification of the PLA, one might prove such as it is implied by the fact that the equations of motion are second order ODEs with boundary conditions (i.e. f = m⋅d2 r/dt2 ), a mathematical proposition implied by another proposition that follows from yet more mathematical statements of physical dynamics.
 
  • #35
Dale said:
What is the criteria used to judge if something has “physical meaning”? The lack of consensus on the answer is probably more due to a lack of consensus about “physical meaning” than about the principle of least action.
I'm sure you meant to say "criterion"! :-)
 
  • #36
Much ado about nothing. Math is not physics. A set of equations is not physics, it is math. The math is used to describe everything that exists, i.e. can be observed. Do some observed objects obey the PLA? If so then PLA has a physical meaning. Meanings are a much harder subject.
 
  • #37
After much more research, I have actually found some literature in which the differences between those who see PLA as having meaning in some sense and those who don't are discussed.

Chris Gray (at the University of Guelph, who wrote the scholarpedia.org article on PLA here) reviews Coopersmith's recent book on PLA, The Lazy Universe (Oxford University Press, 2017), for the American Journal of Physics 86(5):395-398 · May 2018. He says this about PLA's meaning (or, as he says, "justification", which is not quite the same):

"Some (including the author of The Lazy Universe, p. 194) see the justification of Hamilton’s principle in the Feynman path integral of quantum mechanics, which implies Hamilton’s principle in the classical limit. Others feel any justification of classical action principles should be done within the framework of classical mechanics [T. Toffoli, “What is the Lagrangian Counting?” Int. J. Theor. Phys. 42, 363 (2003)]. Many others do not think that the question is relevant and no underlying a priori physical principle exists: the action is not always a minimum, and besides, it is just mathematics since any equation can be reformulated as a variational statement [E. Gerjuoy, A. Rau, and L. Spruch, “A unified formulation of the construction of variational principles,” Rev. Mod. Phys. 55, 725 (1983)]."

Anyway, it seems that this answers my original question about what reasons some might give for thinking PLA does not have a physical meaning (or whatever we want to call it).
 
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  • #38
So do they think it's just luck that it gives the right answer so often? If there is no physical basis and any equation can be formulated in those terms, then it seems like a strange run of luck.
 
  • #39
crastinus said:
After much more research, I have actually found some literature in which the differences between those who see PLA as having meaning in some sense and those who don't are discussed.
You found https://arxiv.org/pdf/1203.2736.pdf several posts ago and that article distinguishes two different concepts for "the" principle of least action. Rather than huff-and-puff about about a principle that is not clearly defined, we could distinguish between those two possibilities.
 
  • #40
crastinus said:
any equation can be reformulated as a variational statement
This is interesting. Did he describe any details about this or list a reference in the footnotes?

I was not aware of that, but I could see how it might work.
 
  • #41
As a schoolboy, I was highly excited about the fact, that so many physical content can be formulated in the most simple form \delta S = 0. Much later I learned, that Lagrange's and Hamilton's representations of classical mechanics treat position and velocity/momentum variables on equal footing. This has led to Gibbs' paradox. The solution is Newton's and Euler's axiomatic of classical mechanics as well as Euler's insight, that the (then often considered to be a theleological reasoning) PLA and the causal description by the equation of motion are equivalent.
Here, not the _second_-order in time equation 'force = mass x acceleration' is fundamental (and is not written down in Newton's 'Principia', indeed), but the _first_-order in time equations
dx = v dt; dv = F/m dt
 
  • #42
crastinus said:
any equation can be reformulated as a variational statement
I think this sounds more significant and profound than it really is. It wouldn't surprise me at all if for any arbitrary equation one can find a mathematical problem that that equation solves. The real question would be whether those problems have anything to do with physics.
 
  • #43
What could the physical meaning of PLA even be?

Well here is one physical meaning. Consider Newton's first law about uniform motion in a straight line? How do you define a straight line? You are assuming that you know what that means, but that basically turns out to be the path an object in uniform motion travels, so it's a bit circular without something more. The alternative of defining it as the shortest distance between two points is one that comes from an action principle that has a definite physical meaning.
 
  • #44
crastinus said:
I have found that some people say “yes, definitely”, and other days “no, definitely not”.

Those who say “no” seem to regard PLA as merely a neat way of packaging the equations. Those who say “yes” seem to regard PLA as somehow fundamental. (There have actually been two recent books on this, Coopersmith’s The Lazy Universe and Albert Rojo’s book, the name of which slips my mind. Both seem to take PLA as fundamental.)

Is there a consensus among physicists that I am unaware of? If not, why not?

What could the physical meaning of PLA even be?

The PLA does not have physical meaning in the sense that it is not always unique. for example, the (classical) Einstein field equations can be derived from several different actions.

https://arxiv.org/abs/gr-qc/9305011
http://www.phy.olemiss.edu/~luca/Topics/gr/action.html
http://www.phy.olemiss.edu/~luca/Topics/gr/action_types.html
http://www.phy.olemiss.edu/~luca/Topics/gr/action_first.html
http://www.phy.olemiss.edu/~luca/Topics/gr/action_vielbein.html
 
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  • #45
If a model makes predictions that are experimentally verifiable, then it has a physical meaning.

But once explanations are found to be equivalent, then it is a beauty contest which one is more fundamental.

Hamiltonian, Lagrangian, and Newtonian descriptions of classical mechanics are equivalent; therefore, there is not a completely scientific way of distinguishing one as "more fundamental." It's a beauty contest.

Likewise, wave and matrix formulations of quantum mechanics are equivalent.
 
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  • #46
Dale said:
This is interesting. Did he describe any details about this or list a reference in the footnotes?

I was not aware of that, but I could see how it might work.

I'm not sure to what extent this is true, but one can search using "inverse problem of the calculus of variations".

https://www.sciencedirect.com/science/article/abs/pii/0020722584900260
Enzo Tonti, Variational formulation for every nonlinear problem

https://bookstore.ams.org/memo-98-473/
Ian Anderson & Gerard Thompson, The Inverse Problem of the Calculus of Variations for Ordinary Differential Equations
 
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  • #47
atyy said:
one can search using "inverse problem of the calculus of variations".
Thanks, that’s perfect!
 
  • #48
The vagueness of the term 'physical meaning' doesn't imply that no such thing exists, it may just mean that it is difficult to simply put into words. In many branches of academia there is a widely used method for solving such issues, namely doing a Delphi method panel study among a group of recognized experts in order to let the issue come to a natural resolution.

crastinus said:
"Some (including the author of The Lazy Universe, p. 194) see the justification of Hamilton’s principle in the Feynman path integral of quantum mechanics, which implies Hamilton’s principle in the classical limit. Others feel any justification of classical action principles should be done within the framework of classical mechanics [T. Toffoli, “What is the Lagrangian Counting?” Int. J. Theor. Phys. 42, 363 (2003)]. Many others do not think that the question is relevant and no underlying a priori physical principle exists: the action is not always a minimum, and besides, it is just mathematics since any equation can be reformulated as a variational statement [E. Gerjuoy, A. Rau, and L. Spruch, “A unified formulation of the construction of variational principles,” Rev. Mod. Phys. 55, 725 (1983)]."
This discussion on the physical content of some equation directly reminds me of what Feynman discussed in his lectures Vol 2, Chp 25-6 (link here, scroll down to part 25-6). I'd copy and paste it here, but its a bit long and I'm not in the mood for converting equations to LaTeX, so just read the entire bit there.

The gist of this seems to be that any equation (or even notation) which experts agree upon on not having any physical content can sometimes seen to still have some as yet unknown physical content (as opposed to purely mathematical content) when viewed from some other point of view. This other point of view can be something like the viewpoint used in another branch of mathematics, perhaps even some mathematical branch unknown to the expert(s) in question but which directly relates to the physics in question possibly even in a novel experimentally unexplored manner; it of course goes without saying that this has happened very often in the course of the history of physics. In other words, whether some piece of mathematics does or does not have any physical content is often a historical path dependent statement.
 
  • #49
Most strongly interacting conformal field theories have no Lagrangian description. If you know the S-Matrix you have completely specified the theory and there isn't a need for a Lagrangian or action. If you can construct realistic field theories without the PLA you might argue that the PLA is not "fundamental" and thus lacks physical meaning.
 
  • #50
quickAndLucky said:
Most strongly interacting conformal field theories have no Lagrangian description. If you know the S-Matrix you have completely specified the theory and there isn't a need for a Lagrangian or action. If you can construct realistic field theories without the PLA you might argue that the PLA is not "fundamental" and thus lacks physical meaning.

Could one likewise argue, "If you can construct realistic theories of mechanics without Newtonian forces, one might argue that Newtonian forces are not "fundamental" and thus lack physical meaning?

If so, how are we going to teach intro physics?
 
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  • #51
atyy said:
The PLA does not have physical meaning in the sense that it is not always unique. for example, the (classical) Einstein field equations can be derived from several different actions.
I have always wondered why physicists prefer actions/Lagrangians over the equations! At the end of the day arn't the equations that matter?
 
  • #52
atyy said:
The PLA does not have physical meaning in the sense that it is not always unique. for example, the (classical) Einstein field equations can be derived from several different actions.

Potentials are not unique either. Does this mean that they do not have a physical meaning?

Physical meaning comes from the predictions made by a model. Being the only model to make those predictions is not a requirement for physical meaning.
 
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  • #53
Dr. Courtney said:
Could one likewise argue, "If you can construct realistic theories of mechanics without Newtonian forces, one might argue that Newtonian forces are not "fundamental" and thus lack physical meaning?

If so, how are we going to teach intro physics?
But, just imagine: someone might invent an entirely different way of describing 'concrete' events in a non Newtonian way which would make sense (perhaps even better sense) to a class of eleven year olds. Bigger paradigm changes have taken place in the past - what a thought!
 
  • #54
sophiecentaur said:
But, just imagine: someone might invent an entirely different way of describing 'concrete' events in a non Newtonian way which would make sense (perhaps even better sense) to a class of eleven year olds. Bigger paradigm changes have taken place in the past - what a thought!

You missed the point. I am disproving the notion that alternate models demonstrate that a given model is not physical. If one accepts the notion that an accurate model needs to be unique to have a physical meaning, then as soon as a phenomenon has two equally accurate models, then neither one of them has a physical meaning. (Or picking which one has the physical meaning is a subjective beauty contest rather than an objective scientific endeavor.) "Making sense" to eleven year olds is a subjective criteria. Paradigm shifts in science come from making better predictions, not by making the same predictions in a way that is more aesthetically pleasing or by making more sense to eleven year olds.
 
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  • #55
Dr. Courtney said:
I am disproving the notion that alternate models demonstrate that a given model is not physical. If one accepts the notion that an accurate model needs to be unique to have a physical meaning, then as soon as a phenomenon has two equally accurate models, then neither one of them has a physical meaning.

That can be problematical. Are Newton/Lagrangian/Hamiltonian approaches different models or different ways to express the same model? Can we make a precise definition of "model?"
 
  • #56
anorlunda said:
That can be problematical. Are Newton/Lagrangian/Hamiltonian approaches different models or different ways to express the same model? Can we make a precise definition of "model?"

I view them as different models which happen to be completely equivalent in terms of testable predictions. (As are matrix and wave quantum mechanics). Newtonian mechanics knows nothing of kinetic energy, potential energy, or action. Does the introduction of kinetic energy, potential energy, and action in later formulations mean forces have no physical meaning? Or do the forces in Newtonian mechanics mean the kinetic energy, potential energy, and action have no meaning in later formulations?

A scientific model is a set of principles that can be used to make testable predictions.

Whether we realize that two models are equivalent does not change their validity or physical meaning. Their physical meaning and validity rest in their ability to make accurate predictions about experiments, not in their uniqueness from other models (either generally, or for specific experiments in question).
 
  • #57
A model is any mathematical description of some phenomenon, usually capturable by some set of differential equations or something mathematically equivalent to that.

The mathematics of Newtonian, Lagrangian and Hamiltonian mechanics are different physical theories but deeply interrelated mathematical procedures, wherein which calculations of a model of the same phenomenon based on these procedures will always lead to the same answers, i.e. the physical theories are in some sense mathematically equivalent. This would be mysterious were it not that they are essentially different aspects of the same theory, namely mechanics, and that the mathematics of mechanics has all these different properties which can each be seperately exploited and further understood independently on their own terms.

The physical content however, i.e. what is intrinsically psychologically implied to the physicist by the mathematics regarding the phenomenon and other analogous phenomenon, of the three approaches are quite distinct and these distinctions can themselves suggest different ways of modifying concepts of the theory in order to generalize to some grander theory; in theoretical science, these modifications and generalizations can lead to very different kinds of theories, which aren't necessarily equivalent anymore to some other theories after such a modification is made compared to the situation before the modification was made where the theories were equivalent.

Feynman, having as usual already thought about these issues extensively, explains this marvelously in a matter of minutes here:
 
  • #58
Dr. Courtney said:
Potentials are not unique either. Does this mean that they do not have a physical meaning?

Physical meaning comes from the predictions made by a model. Being the only model to make those predictions is not a requirement for physical meaning.

Yes, that's exactly what I was thinking of. It is quite conventional to say within classsical electrostatics that potentials themselves are not physically meaningful, because they are not unique. Rather it is the potential difference that is physically meaningful.

One can choose to use other language, but this choice is very reasonable.
 
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  • #59
Dr. Courtney said:
I am disproving the notion that alternate models demonstrate that a given model is not physical.
Dr. Courtney said:
Paradigm shifts in science come from making better predictions, not by making the same predictions in a way that is more aesthetically pleasing or by making more sense to eleven year olds.
I was rather assuming that the necessity of Physicality would apply to individuals with only Concrete Cognitive skills. From this
Dr. Courtney said:
If so, how are we going to teach intro physics?
I thought you were thinking along the same lines.
My view of the term 'physical' is that an idea is readily accepted in terms of already familiar and very concrete terms. By definition, a Physical explanation excludes factors that are new to the learner. One has only to examine one's own appreciation of Physics (and a lot of other stuff, of course) to realize that 'Physical' is mostly synonymous with 'familiar'.
Physical descriptions include "Nature abhors a vacuum" and 'the music of the spheres' and we have advanced beyond them by using notions of pressure and gravitational laws which would have been very non-physical at one time.
 
  • #60
Another example: the choice of a coordinate system is part of a physical model from the earliest physics courses. Dropping a rock from tower. Is y = 0 m the starting position or the ending position? The choice impacts the model, and while the two models are equivalent (make the same predictions), they are different models.

At some point (early, I hope) those who practice physics realize that there are no right or wrong choices of coordinate systems, though the math is sometimes easier or harder as a result of our choices. But the fact that the choice of coordinate system is not _unique_ does not mean that the choice of coordinate system (and the resulting mathematical models) do not have physical meaning. Of course, the choice of coordinate system has a physical meaning.
 
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