Conservation laws in Newtonian and Hamiltonian (symplectic) mechanics

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SUMMARY

In the discussion on conservation laws in Newtonian and Hamiltonian mechanics, it is established that Newtonian mechanics conserves momentum and angular momentum through Newton's laws and central forces, while Hamiltonian mechanics connects conservation laws to symmetries via one-parameter Lie groups and symplectic flows. The Hamiltonian framework is noted to be less general than Newtonian mechanics due to its exclusion of dissipative forces. The Noether theorem is highlighted as a key principle linking symmetries to conserved quantities, emphasizing the non-uniqueness of Hamiltonians in describing the same system. Ultimately, the discussion contrasts the completeness of Newtonian mechanics with the limitations of Hamiltonian mechanics.

PREREQUISITES
  • Newton's laws of motion
  • Hamiltonian mechanics
  • Symplectic geometry
  • Noether's theorem
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  • Study the implications of Noether's theorem in classical mechanics
  • Explore the role of symmetries in Hamiltonian mechanics
  • Investigate dissipative forces and their impact on conservation laws
  • Learn about the mathematical foundations of symplectic geometry
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Physicists, mathematicians, and students of mechanics interested in the foundational principles of classical mechanics and the relationship between symmetries and conservation laws.

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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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