Comparing Lagrange's Equation of Motion and Euler-Lagrange Equations

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Discussion Overview

The discussion focuses on the differences between Lagrange's equation of motion and the Euler-Lagrange equations, exploring their formulations and applications within classical mechanics, particularly in the context of the Hamiltonian and Lagrangian formulations of mechanics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants suggest that Lagrange's equations of 2nd kind correspond to the Euler-Lagrange equations derived from the Hamilton least-action principle in its Lagrangian formulation.
  • Others clarify that the Lagrange equations of 1st kind are related to the Euler-Lagrange equations under constraints.
  • A participant seeks confirmation on the formulation of the Lagrange equations of 2nd kind and provides a mathematical expression.
  • Another participant corrects the formulation of Hamilton's equations related to the Lagrange equations of 2nd kind.
  • There is a discussion about the formulation of the Lagrange equations of 1st kind, with a participant noting that these are typically expressed in Cartesian coordinates and involve Lagrange multipliers to account for constraints.
  • A participant reflects on their understanding of the Euler-Lagrange equations in the context of fields versus 1D systems.

Areas of Agreement / Disagreement

Participants express differing views on the formulations and interpretations of the Lagrange equations of 1st and 2nd kind, indicating that multiple competing views remain without a clear consensus.

Contextual Notes

There are references to specific mathematical formulations and the role of constraints, but the discussion does not resolve the nuances of these formulations or their implications in different contexts.

Niles
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Hi

What is the difference between Lagrange's equation of motion and the Euler-Lagrange equations? Don't they both yield the path which minimizes the action S?


Niles.
 
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The Lagrange Equations of 2nd kind are the Euler-Lagrange equations of the Hamilton least-action principle in its Lagrangian formulation. In the Hamiltonian formulation you get the equivalent Hamilton Canonical Equations of Motion for configuration and conjugate momentum variables.

The Lagrange Equations of 1st kind are the Euler-Lagrange equations of the Hamilton least-action principle under constraints.
 
Just to be absolutely sure, then by the Lagrange Equations of 2nd kind you mean

[tex] \frac{d}{{dt}}\left( {\frac{{\partial L}}{{\partial v_i }}\left( {\gamma (t),\mathop \gamma \limits^. (t),t} \right)} \right) - \frac{{\partial L}}{{\partial q_i }}(\gamma (t),\mathop \gamma \limits^. (t),t) = 0[/tex]

where the corresponding Hamilton's equations are[tex] \begin{array}{l}<br /> \mathop q\limits^. _i (t) = \frac{{\partial H}}{{\partial p_i }}(q(t),p(t),t) \\ <br /> \mathop p\limits^. _i (t) = - \frac{{\partial H}}{{\partial p_i }}(q(t),p(t),t)<br /> \end{array}[/tex]

?
 
Yep, but the last Eq. should read

[tex]\dot{p}_i=-\frac{\partial H}{\partial q^i}.[/tex]
 
Great -- and for clarity, then by the Lagrange Eqations of the 1st kind you mean

[tex] \frac{d}{{dt}}\left( {\partial _{\mathop x\limits^. } L} \right) - \partial _x L = 0[/tex]

?Niles.
 
No, these are the Lagrange equations of 2nd kind. Those of 1st kind are usually formulated in Cartesian coordinates taking into account constraints with help of Lagrange multipliers. These introduce the forces needed to fulfill the constraints explicitly into the equations of motion.
 
Ahh, I see. In that case I believe I have deciphered what my book means: The first EL-equations I wrote are for fields, where the ones I wrote in #5 are in 1D.
 

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