Lagrange & Hamiltonian mech => Newtonia mech.

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Discussion Overview

The discussion revolves around the relationship between Lagrangian, Hamiltonian, and Newtonian mechanics, specifically whether every classical mechanics problem solvable by Lagrangian and Hamiltonian methods can also be solved using Newtonian methods. Participants explore the perceived ease of Lagrangian and Hamiltonian approaches compared to Newtonian methods, considering various contexts such as computational difficulties and specific system types.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that all classical mechanics problems solvable by Lagrangian and Hamiltonian methods are also solvable by Newtonian methods, but they acknowledge potential computational or analytical difficulties.
  • Others argue that the principle of least action provides a more convenient framework for expressing the action of a system in generalized coordinates, which may simplify the analysis compared to Newtonian methods.
  • A later reply questions the generality of the perceived simplicity of Lagrangian methods, noting that in certain cases, such as dissipative systems, finding a suitable Lagrangian can be complex.
  • It is suggested that the choice of formulation often depends on the specific problem at hand, as each method may present its own challenges.

Areas of Agreement / Disagreement

Participants do not reach a consensus; multiple competing views remain regarding the equivalence of the methods and the conditions under which one may be preferred over the others.

Contextual Notes

Limitations include potential assumptions about the nature of the systems being discussed, as well as the dependence on specific problem contexts that may affect the choice of method.

MathematicalPhysicist
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My question is simple is every classical mechanics problem which is solvable by Lagrangian & Hamiltonian methods also solvable by Newtonian methods of forces and torques?

And why does it seem that LH make solutions to be a lot more easier than Newtonian methods, and is it always this way?
 
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The principle of least action is the common description of all physical theories at a fundamental level. All fundamental theories are most simply described as such a variational principle (standard model of elementary particle physics, classical field theory (e.g., classical electromagnetics, general relativity), and point-particle mechanics).

The reason for this is that it most easily allows to study symmetries of the fundamental laws of nature, such as space-time symmetries (Galileo, Poincare, general covariance) and external symmetries leading to conservation laws for engery, momentum, angular momentum, center-of-mass velocity, and various charge-like quantities (electrical charge, baryon number, lepton number, etc.), respectively.

Of course, on the classical (i.e., non-quantum) level of point-particle mechanics, the action principle is equivalent to the Newton (or relativistic if necessary) equations of motion for the particle, and you can of course write down this equations from the very beginning.

What makes the action principle more convenient from a practical point of view is that it is way easier to express the action (or the Lagrangian/Hamiltonian) of the system in general coordinates, adapted to the problem at hand, than using directly the equations of motion and performing the transformation from Cartesian to generalized coordinates.
 
MathematicalPhysicist said:
My question is simple is every classical mechanics problem which is solvable by Lagrangian & Hamiltonian methods also solvable by Newtonian methods of forces and torques?

And why does it seem that LH make solutions to be a lot more easier than Newtonian methods, and is it always this way?

If by "classical" you mean non-relativistic classical, then the three formulations are formally equivalent. You can, however, find computational or analytical difficulties. That is why one chooses the formulation more adequate to the problem.
 
It only <seems> that way, well said. Indeed, the lagrangian methods seem simpler, but in some cases, they are really not (here I mean dissipative systems, where the task to find a lagrangian is not simple). It normally all boils down to solving ODE's. To get to them can be simpler using one method or another, but it's not a general rule.
 

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