Designing an Invariant Lagrangian: Rules and Considerations

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    Lagrangian Writing
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SUMMARY

The discussion centers on the essential rules for designing an invariant Lagrangian in classical mechanics. Key requirements include the Lagrangian being a function of position and its first-order derivatives, ensuring the action is a scalar for trajectory agreement, and avoiding high-order derivatives to prevent non-locality. Additionally, the action must maintain invariance under Galilei transformations for Newtonian mechanics or Poincaré transformations for special relativity. Proper generalized coordinates and their constraints must also be incorporated into the formulation.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with Galilei and Poincaré transformations
  • Knowledge of generalized coordinates and constraints
  • Basic principles of classical mechanics
NEXT STEPS
  • Study the formulation of Lagrangians in classical mechanics
  • Explore the implications of invariance under Galilei transformations
  • Investigate the role of generalized coordinates in Lagrangian mechanics
  • Learn about the first variation of the action and its significance
USEFUL FOR

The discussion is beneficial for physicists, particularly those specializing in classical mechanics, theoretical physicists designing models, and students studying advanced mechanics concepts.

accdd
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What are the rules for writing a good Lagrangian?
I know that it should be a function of the position and its first order derivatives, because we know that we only need 2 initial conditions (position and velocity) to uniquely determine the future of the particle.
I know that the action has to be a scalar because everyone has to agree on the trajectory the particle travels.
I know that high-order derivatives must be avoided to avoid non-locality.
What else?
 
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Be sure to include the appropriate generalized coordinates and list the constraints relating them.
 
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In addition to the very general properties you listed, you should make the action (or more precisely the first variation of the action) invariant under Galilei (Newtonian mechanics) or Poincare (special relativistic mechanics) transformations.
 
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