Conservation laws in Newtonian and Hamiltonian (symplectic) mechanics

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Discussion Overview

The discussion centers on the comparison of conservation laws in Newtonian mechanics versus Hamiltonian mechanics, exploring the relationship between these laws and symmetries. It examines theoretical implications, mathematical foundations, and the generality of each framework.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants argue that conservation laws in Newtonian mechanics arise from Newton's laws and the assumption of central forces, while noting that this framework does not address symmetries.
  • Others propose that in Hamiltonian mechanics, conservation laws are inherently linked to symmetries, specifically through the action of symplectic groups on phase space.
  • A participant questions the assertion that Hamiltonian mechanics is less general than Newtonian mechanics, suggesting that Hamiltonian mechanics serves as a complete description of Newtonian mechanics.
  • Another participant challenges the need to choose between the two frameworks, using an analogy about tools to illustrate the point.
  • There is a call for proof regarding the claim that Hamiltonian mechanics is the complete description of Newtonian mechanics, with a subsequent assertion that such a proof is not possible.

Areas of Agreement / Disagreement

Participants express differing views on the generality of Hamiltonian mechanics compared to Newtonian mechanics, with no consensus reached on the completeness or superiority of either framework.

Contextual Notes

The discussion involves assumptions about the nature of symmetries and the definitions of completeness in mechanics, which remain unresolved. The implications of Noether's theorem and the uniqueness of Hamiltonians are also points of contention.

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In Newtonian mechanics, conservation laws of momentum and angular momentum for an isolated system follow from Newton's laws plus the assumption that all forces are central. This picture tells nothing about symmetries.

In contrast, in Hamiltonian mechanics, conservation laws are tightly connected to symmetries. A symmetry is a one-parameter Lie group with a symplectic group action on phase space that preserves Hamiltonian (a Hamiltonian-preserving symplectic flow), and the infinitesimal generator of this flow is a conserved quantity.

However, the standard symplectic Hamiltonian description is less general than Newton's law because dissipative forces aren't incuded. So, it seems that Newton's conservation laws are more general then the Hamiltonian ones. Is there any attempt for achieving the same generality by symmetry considerations, as Newtonian description have?
 
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Why do you think the Hamiltonian description is less general? On a fundamental level, it's the complete description of Newtonian mechanics, which is a mathematically closed system (in contradistinction to relativistic point-particle mechanics, which is not as complete, but that's another story).

BTW: The most general form of the quoted Noether theorem (according to which each (global) one-parameter Lie symmetry defines a conserved quantity and vice versa) makes the much weaker assumption that only the variation of the action must stay invariant. This exhausts automatically the fact that for the dynamics of a given system the Hamiltonian is not unique, but there are many equivalent Hamiltonians describing the same system.
 
Why do you have to choose at all? If you buy a screwdriver does that mean you have to stop using your hammer?
 
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vanhees71 said:
On a fundamental level, it's the complete description of Newtonian mechanics
This is a mathematical statement. Can you prove it?
 
That's a physical statement, and of course you can't prove it.
 

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