Are lagrangians based on physical observation or mathematics?

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Discussion Overview

The discussion revolves around the nature of Lagrangians in physics, specifically whether they are derived from physical observations or mathematical reasoning. It explores the derivation of Lagrangians in classical mechanics, quantum mechanics, and quantum field theory, as well as the challenges in determining appropriate Lagrangians for specific problems.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question whether Lagrangians are based on physical observation or mathematical reasoning.
  • One participant suggests that the formulation of a Lagrangian often seems to be a matter of trial and error, rather than a standardized procedure.
  • Another participant states that in classical mechanics, the Lagrangian is simply the difference between kinetic and potential energy (L = T - V), and this concept is extended in quantum mechanics and quantum field theory.
  • A different viewpoint emphasizes that the equivalence of Newtonian and Lagrangian dynamics can be proven, suggesting that the Lagrangian formulation is a reformulation of mechanics rather than a mysterious process.
  • One participant notes that while the Lagrangian minimizes the time integral of action, this does not necessarily help in finding the correct Lagrangian for a given problem, especially in quantum field theory.
  • A participant expresses curiosity about the coupling of fields, indicating a desire for clarification on how coupling constants are used in this context.

Areas of Agreement / Disagreement

Participants express differing views on the derivation and nature of Lagrangians, with no consensus reached on whether they are fundamentally based on physical observation or mathematical reasoning. The discussion remains unresolved regarding the methods for deriving appropriate Lagrangians in various contexts.

Contextual Notes

Participants mention the challenges of deriving Lagrangians in quantum field theory compared to classical mechanics, highlighting the complexity and effort involved in finding suitable formulations.

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are lagrangians based on physical observation or mathematical reasoning?
 
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yes.
 
In the same question, "Why do we use THIS Lagrangian, or THAT, and HOW did we derive it?", I have been told that "it just suits the corresponding problem, it just works out!".

I guess that the first one who came up with a working Lagrangian had tried a lot, before he got there. One may be able to recognize several proper terms in a Lagrangian, such as the kinetic terms, or mass terms, or interactions between the sources and the fields, which have imply physical meaning. But I don't think there is a "standard" way to create a working Lagrangian, or a step by step proof of the procedure to get there!
 
in classical mechanics L = T-V, kinetic energy - potential energy of the system.
in QM, and QFT we just push this idea further
 
PhysiSmo said:
In the same question, "Why do we use THIS Lagrangian, or THAT, and HOW did we derive it?", I have been told that "it just suits the corresponding problem, it just works out!".
I am not sure what you are driving at when you say "it just works out".
It is not a difficult matter to prove the equivalance of Newtonian and lagrangian dynamics. You can find this proof in just about all undergraduate classical mechanics texts, see Marion. Given this proof, it doesn't just work out for some mysterious reason, rather it is simply a reformulation of mechanics in terms of energy instead of forces. If anything about the langrangian is mysterious, I would consider it to be the fact that the langrangian formulation implies that nature always minimizes the time integral of action. Which is a topic that has been beat to death on this forum with no real consensus.
 
When I answered the original question posted, the thread was in the "Quantum Mechanics" section, not the "Classical Mechanics" that has been moved now.

Anyway, in C.M., Lagrangian is always L= T - V, and one can derive it easily. In QFT, one cannot use a similar path, since, as far as I know, it doesn't exist.

The fact that the Lagrangian minimizes the time integral action does not push one further to find the correct corresponding Lagrangian to his problem.

Say, i.e., we need to find the Lagrangian from which Klein-Gordon equation arises. We cannot "prove" the satisfying Lagrangian by means of a "law", such as T-V, as in C.M., but only by means of minimizing the action time integral. Which means that the procedure requires a lot of effort, trying and fantasy to get the proper result!
 
i am curious to know how can you couple the field A with the dirac field with the use of a coupling constant. I am not quite sure how that works out?
 

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