System and phase space trajectory

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SUMMARY

Phase space trajectories serve as geometric representations of classical systems, but they do not fully specify these systems. For instance, the trajectory defined by the equation x² + p² = 1 for a one-dimensional harmonic oscillator leaves ambiguity in initial conditions, such as x(t=0)=0 or x(t=0)=1. A trajectory is defined as a continuous map from an interval in the real numbers to its range, distinguishing it from mere curves. Ultimately, while phase space provides a framework, the equations of motion can directly yield the same trajectories without necessitating phase space representation.

PREREQUISITES
  • Understanding of classical mechanics and harmonic oscillators
  • Familiarity with phase space concepts and trajectories
  • Knowledge of parametrization in mathematical functions
  • Basic grasp of the Dirac-Von Neumann axioms in physics
NEXT STEPS
  • Explore the mathematical foundations of phase space in classical mechanics
  • Study the role of parametrization in defining trajectories
  • Investigate the Dirac-Von Neumann axioms and their implications for classical systems
  • Learn about the equations of motion and their solutions in various physical contexts
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Physicists, students of classical mechanics, and anyone interested in the mathematical representation of physical systems will benefit from this discussion.

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To what extent do phase space trajectories describe a system? I often see classical systems being identified with (trajectories in) phase space, from which I get the impression these trajectories are supposed to completely specify a system. However, if you take for example the trajectory x^2+p^2=1 for a one-dimensional harmonic oscillator, it is still left open if x(t=0)=0 or x(t=0)=1 which corresponds to two different parameterizations of the circle. This leads me to ask: what is the role of phase space trajectories in the description of physical systems?
 
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A phase trajectory, by definition, includes a particular parametrization in its specification. It's a path through configuration space, with a path being defined as a continuous map from an interval in the real numbers to the path's range. So, ##x^2 + y^2 = 1## isn't a trajectory, it's just a curve. A corresponding trajectory would be ##t\in[0,1) \rightarrow (\cos t, \sin t)##, etc. You can always reparametrize, but then you have a different trajectory.
 
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I see. So there really isn't any need for the concept of phase space for describing physical systems, since the trajectory can be found by just solving the equation of motion directly. My question was motivated by the classical variant of the Dirac-Von Neumann axioms where a classical system is associated with phase space, but maybe I'm reading too much into it.
 
Trajectories in phase space are just geometric representations of the solutions to the equations of motion. It's not one or the other, they're interchangeable.
 

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