Lagrangian Mechanics Question: How do we get the T and V terms?

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Discussion Overview

The discussion centers on the definitions and derivations of the kinetic (T) and potential (V) energy terms in Lagrangian Mechanics, exploring their relationship to Newtonian mechanics. Participants examine how these terms are established and their implications for the formulation of mechanics.

Discussion Character

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

Main Points Raised

  • One participant questions whether T is defined as 1/2mv^2 and expresses concern about deriving it using the work-energy theorem, feeling it relies on Newtonian principles.
  • Another participant confirms that T is indeed defined as 1/2mv^2 but notes that V is only defined for conservative forces, suggesting that non-conservative forces require different Lagrangian forms.
  • A different perspective suggests that T and V can be seen as undiscussed assumptions from which Newton's laws can be derived, while also allowing exploration of alternative choices for T and V to enrich mechanics beyond Newtonian frameworks.
  • Historical context is provided, indicating that the Newtonian formulation predates the concepts of kinetic energy and that the Lagrangian and Hamiltonian frameworks offer broader applicability, suggesting a progression in the understanding of mechanics.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and derivations of T and V, with no consensus reached on how these terms should be established or their implications in the context of Lagrangian Mechanics versus Newtonian Mechanics.

Contextual Notes

Participants acknowledge that the definitions of T and V may depend on the context of conservative versus non-conservative forces, and there are unresolved questions regarding the historical development of these concepts in physics.

McLaren Rulez
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According to my CM text, Lagrangian Mechanics can be used to derive Newton's laws. We define the Lagrangian as L=T-V.

Now, how do we know what T is? Is it defined to be 1/2mv^2? The only way I know how to derive that is using the work energy theorem which feels like 'cheating' since I am sort of using the Newtonian formulation of things to get it.

Similarly, how do we find the potential? The way it is done in regular Newtonian mechanics is by showing that curl of F is zero and hence we can find a potential function from the original force. For Lagrangian Mechanics, is the potential thought of as the fundamental quantity that is always given (like the way the force is given in Newtonian Mechanics)?

Thank you
 
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Well, yes.

T is defined to be [tex]\frac{1}{2}m\dot{\textbf{r}}^2[/tex]

V however is defined only for conservative forces. One cannot write a Lagrangian of the form T-V for non-conservative forces. However, there are other forms of the Lagrangian that can be used in such situations (I remember learning this when I did classical mechanics, but am unclear now what exactly this was. I'll read it up and reply back).
 
McLaren Rulez said:
According to my CM text, Lagrangian Mechanics can be used to derive Newton's laws. We define the Lagrangian as L=T-V.

Now, how do we know what T is? Is it defined to be 1/2mv^2?

Starting with Newton's mechanics (as undiscussed assumptions), one finds that one can encode it all into a Lagrangian where T is the sum of all kinetic energies of the particles and V the sum of all potential energies.

Conversely, one may start with these formulas for T and V (as undiscussed assumptions) and derive Newton's laws. However, one can then explore what different choices for T and V imply and gets a much richer and more flexible mechanics as Newton's. Thus one learns Newton to get a start, and then learns the much more powerful Lagrangian and Hamiltonian frameworks to do more modern stuff.
 
McLaren Rulez said:
We define the Lagrangian as L=T-V.

Now, how do we know what T is? Is it defined to be 1/2mv^2? The only way I know how to derive that is using the work energy theorem which feels like 'cheating' since I am sort of using the Newtonian formulation of things to get it.

Well, historically the Newtonian formulation came first. The Newtonian formulation is momentum oriented. The concept of kinetic energy did not become a regular part of the physicist's toolbox until much, much later.

As Neumaier mentions, the Lagrangian and Hamiltonian frameworks are more versatile, they have a wider range of deployment.

The cases where the Newtonian formulation is suitable form a subset of the sets of cases where a Lagrangian/Hamiltonian framework is suitable. I suppose that that is why some authors describe that 'Newtonian dynamics can be derived from Lagrangian mechanics'. In the sense that the Newtonian formulation has been eclipsed by the Lagrangian/Hamiltonian formulation that is in itself a true statement.

But historically it was the lessons learned from the Newtonian formulation that prepared the physics community for arriving at Lagrangian/Hamiltonian mechanics.
 

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