Geometry of phase space and extended phase space

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SUMMARY

The discussion centers on the geometrical interpretation of phase space and extended phase space in the context of ordinary differential equations (ODEs), specifically using the example of a free-falling particle described by the equations \(\dot{x} = v\) and \(\dot{v} = -g\). It is established that the phase curves in this autonomous system are parabolas, and that the dimension of its phase space is 2, indicating no extended phase space is applicable. When time is explicitly included, the system can be transformed into a non-autonomous one, thereby increasing the dimension of the phase space and introducing the concept of extended phase space.

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  • Understanding of ordinary differential equations (ODEs)
  • Familiarity with phase space concepts in classical mechanics
  • Knowledge of autonomous and non-autonomous systems
  • Basic grasp of vector fields and their projections
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  • Study the transformation of non-autonomous systems into autonomous systems
  • Explore the concept of extended phase space in more complex dynamical systems
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Coto
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I just want to clarify the geometrical interpretation of these objects as encountered in the basic theory of ODEs.

For discussion let's use the simple set of differential equations found in classical mechanics for a free falling particle:

\dot{x} = v;\ \ \dot{v} = -g;

Now in phase space the phase curves are simply parabolas (as can easily be seen). How about extended phase space then?

Are the phase curves simply the projection of integral curves in the extended phase space onto the position-velocity plane?

Are phase velocity vector fields the projection of a direction field in extended phase space onto the position-velocity plane?

Thanks in advance,
Coto
 
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Hi Coto,

Coto said:
Now in phase space the phase curves are simply parabolas (as can easily be seen). How about extended phase space then?
Your example is an autonomous system (does not depend on time explicitly), therefore
the dimension of its phase space is 2 (i.e. there is no extended phase space for this problem).
When time enters the problem explicitly (for example, as in a forced system), the non-autonomous system
x'=f(x,t)
can be rewritten as an autonomous one with an increase in the dimension of the phase space (this is the so-called extended phase space)
x'=f(x,y)
y'=1

Mathador
 

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