Is the Lagrangian a kind of Energy

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Discussion Overview

The discussion centers around the relationship between the Lagrangian and energy, particularly in the context of classical mechanics and quantum mechanics. Participants explore whether the Lagrangian can be interpreted as a form of energy and the implications of various potential forms in Lagrangian mechanics.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant suggests that if the Lagrangian is expressed as L=T-V, then substituting V(-x)=-V(x) could lead to insights about quantizing particle dynamics using Lagrangians as a form of pseudo-energy.
  • Another participant counters that Lagrangians are not observables and should not be considered as "pseudo" energy, emphasizing their utility as a tool in quantum physics.
  • A question is posed regarding the implications of applying the Lagrangian to a quantum wave function, indicating uncertainty about the relevance of eigenstates of the Lagrangian in classical mechanics.
  • It is noted that while the Lagrangian can be measured through kinetic and potential energy, the action is the more significant physical quantity, which is derived from the Lagrangian.
  • One participant raises a question about distinguishing between energy and Lagrangian without prior knowledge of the system, suggesting that the minimum principle could be reformulated with a modified Hamiltonian.
  • Another participant points out that the Hamiltonian's relationship to the Lagrangian is not straightforward, particularly in cases like magnetic phenomena.
  • There is a correction regarding the Hamiltonian in general relativity, with a participant asserting that it is not zero and referring to the ADM Hamiltonian formulation.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the Lagrangian and its relationship to energy, with no consensus reached on whether the Lagrangian can be considered a form of energy or how it should be interpreted in various contexts.

Contextual Notes

Some discussions involve assumptions about the definitions of energy and Lagrangian, and there are unresolved questions regarding the applicability of certain principles in different physical contexts, such as general relativity.

Kevin_spencer2
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If we have that Lagrangian is equal to L=T-V and Hamiltonian is just H=T+V my question is if for every lagrangian we could consider is just the energy of a particle with a potential -V(x) instead of V(x) what would happen if V(-x)=-V(x)?

In fact if we substitute velocities by momenta in the Lagrangian the Euler-Lagrange equation for a particle is just (putting -V(x) instead of V(x)) the Hamilton equation [tex]\dot p =-\frac{dH}{dp}[/tex].

then it occurred to me if we could use this fact to quantizy the dynamics of a particle using Lagrangians as if they were the pseudo-energy of the system to get energy levels.
 
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Nope, it doesn't work that way. Lagrangians are not observables, they cannot be measured. There's nothing "pseudo" about them. Their unit is energy, just like for a Hamiltonian, but nothing more. They're just a tool. Very useful in quantum physics, i must say.

Daniel.
 
then, what would we get if we put [tex]L(p,q)|\Phi >[/tex] where our [tex]\Phi[/tex] is just the wave function of a quantum system
 
Kevin_spencer2 said:
then, what would we get if we put [tex]L(p,q)|\Phi >[/tex] where our [tex]\Phi[/tex] is just the wave function of a quantum system

I'm not sure why you'd want the eigenstates of the lagrangian. It's certainly observable, but I think that's beyond the point of this thread (being in classical mechanics). I personally have never seen it used, which doesn't mean that it's not of value, it's just that lagrangians enter quantum mechanics in a way that is a little independent of state vectors.

You can measure the lagrangian by just measuring the kinetic and potential energy, certainly. But the physical quantity of most interest is the action, which is just [tex]S = \int_t L(q, \dot{q},t)[/tex], and which is the basis for a lot of least-action principles, etc.
 
- the question is without prior knowledge of the system if they give you a quantity [tex]F(\dot q , q)[/tex] how could you know if you've got the energy of the whole system or just the Lagrangian?, in fact you could write the minimum-principle in the form [tex]S=\int_{a}^{b}dt \mathcal H(q,\dot q, t)[/tex] where H has -V(x) instead of V(x), the question is that it's easier to work with Lagrangians rather than Hamiltonians, and that for example the Lagrangian for GR is just [tex](-g)^{1/2}R[/tex], however the Hamiltonian is just 0, which arises to lots of problems.
 
The hamiltonian need not equal T + V; it depends on the form of the lagrangian. The lagrangian is also not, generally, T - V -- look to magnetic phenomena to confirm this.
 
Kevin_spencer2 said:
- the question is without prior knowledge of the system if they give you a quantity [tex]F(\dot q , q)[/tex] how could you know if you've got the energy of the whole system or just the Lagrangian?, in fact you could write the minimum-principle in the form [tex]S=\int_{a}^{b}dt \mathcal H(q,\dot q, t)[/tex] where H has -V(x) instead of V(x), the question is that it's easier to work with Lagrangians rather than Hamiltonians, and that for example the Lagrangian for GR is just [tex](-g)^{1/2}R[/tex], however the Hamiltonian is just 0, which arises to lots of problems.

The Hamiltonian is not 0 for GR, search for ADM Hamiltonian formulation of general relativity.

Daniel.
 

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