Ad Hoc Lagrangians: Physics & Variational Formulation

  • Context: Graduate 
  • Thread starter Thread starter ShayanJ
  • Start date Start date
  • Tags Tags
    Lagrangians
Click For Summary

Discussion Overview

The discussion revolves around the use of Lagrangian mechanics, particularly the formulation of Lagrangians in cases where they do not take the standard form of \( L = T - V \). Participants explore the implications of defining Lagrangians that yield known equations of motion and question the necessity and foundational aspects of such formulations in both classical mechanics and quantum field theory (QFT).

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions the utility of deriving Lagrangians that reproduce known equations of motion, suggesting it seems nonsensical to derive something already known.
  • Another participant emphasizes that the Lagrangian is typically defined as \( L = T - V \), while noting that the Hamiltonian does not always follow the form \( H = T + V \).
  • Some participants express interest in understanding why the Lagrangian approach is considered more fundamental, given that it often appears to be a method for obtaining known results.
  • A participant mentions that the significance of the Lagrangian may not be clear until one studies more advanced topics in QFT, where field equations are derived from fundamental principles rather than assumed.
  • There is a suggestion that it may be useful to derive Lagrangians in classical mechanics without prior knowledge of the equations of motion, to explore foundational principles.
  • Another participant agrees that deriving Lagrangians from fundamental principles can be both possible and useful.
  • One participant highlights that once a system is expressed in Lagrangian form, it allows for the exploration of additional aspects such as symmetries and generalizations that may not be evident from the equations of motion alone.

Areas of Agreement / Disagreement

Participants express a range of views regarding the utility and foundational nature of Lagrangians, with some questioning their necessity in reproducing known results, while others advocate for their exploration in both classical mechanics and QFT. The discussion remains unresolved with multiple competing perspectives present.

Contextual Notes

Participants note that the understanding of Lagrangians may depend on the context of classical mechanics versus quantum field theory, and that assumptions about the equations of motion can influence the discussion. There is also an acknowledgment of the limitations in understanding the foundational aspects of Lagrangian mechanics without delving into more complex theories.

ShayanJ
Science Advisor
Insights Author
Messages
2,802
Reaction score
605
Lagrangian mechanics, as you know, is very useful in today's physics. But there is a point that I can't understand.
In cases where we can write L=T-V, Lagrangian mechanics is very useful because for some problems, it gives us a easier way than Newtonian mechanics to derive the equations of motion.
But in cases where we can't write L=T-V, it seems that people just look for a Lagrangian to give the right equations of motion. But that is useless!
For example, we know that for Newtonian gravity we have \nabla^2 \Phi=4\pi G \rho and look for a Lagrangian density to give that same equation and after finding it, they say we have the variational formulation of Newtonian gravity. My question is, why not just use the equation we know? Why should we use something we know to derive something that gives the same thing we knew? That seems non-sense!
Of course its useful for something we're just trying to understand. I mean, when we have no law for some system, we can look for something in it that always gets extremum and then find a variational theory for it and then find the laws of motion.
 
Physics news on Phys.org
As far as I know, the Lagrangian is defined as ##L=T-V##. On the other hand, the hamiltonian in not always ##H=T+V##, even though it usually is.
 
hilbert2 said:
As far as I know, the Lagrangian is defined as ##L=T-V##. On the other hand, the hamiltonian in not always ##H=T+V##, even though it usually is.

So you don't know far enough!
Check here!
Another example is the Lagrangian for interaction of a classical charged particle with electromagnetic field.
 
Last edited:
I don't have an answer to this question, but I just want to mention that I'm interested in it too and I've been waiting for some answers to show up. People say that the Lagrangian approach is somehow "more fundamental," yet the Lagrangian seems to be defined as "something that gives you the right answer." It really seems like there's a piece missing.

Hopefully bringing this back up will stir up some responses...
 
thegreenlaser said:
I don't have an answer to this question, but I just want to mention that I'm interested in it too and I've been waiting for some answers to show up. People say that the Lagrangian approach is somehow "more fundamental," yet the Lagrangian seems to be defined as "something that gives you the right answer." It really seems like there's a piece missing.

If your only exposure to Lagrangian mechanics is through classical mechanics then your viewpoint is fortunately very common amongst students. Indeed at that point it would seem like we just come up with a Lagrangian that gives us the field equations we already knew a priori so the question arises: what's even the point of the Lagrangian, apart from computational facility, given that it is claimed to be more fundamental?

Unless you study more esoteric aspects of classical field theory the answer to this will probably not become apparent on a practical level until you study QFT. The point there is we do not know the field equations beforehand, it has to be actually derived from more fundamental principles of QFT. Indeed we use a very powerful tool called local gauge invariance (or just gauge invariance), along with renormalization, to basically heavily constrain and subsequently guess the Lagrangian for a field theory and from it calculate the field equations.
 
WannabeNewton said:
Unless you study more esoteric aspects of classical field theory the answer to this will probably not become apparent on a practical level until you study QFT. The point there is we do not know the field equations beforehand, it has to be actually derived from more fundamental principles of QFT. Indeed we use a very powerful tool called local gauge invariance (or just gauge invariance), along with renormalization, to basically heavily constrain and subsequently guess the Lagrangian for a field theory and from it calculate the field equations.

Is it possible/useful to do a similar thing in classical mechanics? (I.e., pretend that we don't know the equations already and force ourselves to derive the Lagrangian from more fundamental principles.)
 
thegreenlaser said:
Is it possible/useful to do a similar thing in classical mechanics?

Yes it is possible and often useful.
 
Once you can cast something in a certain form (for example, a Lagrangian),
then you can use the machinery developed to study other aspects that may not be apparent from just the equation of motion (for example: symmetries, generalizations (including dimensionality quantization, etc) , symmetry-preserving computational schemes, recognizing analogies, etc).
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 19 ·
Replies
19
Views
5K
  • · Replies 17 ·
Replies
17
Views
2K
Replies
9
Views
2K
  • · Replies 20 ·
Replies
20
Views
3K
Replies
1
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K