Is Time Evolution in Phase-Space Equivalent to Canonical Transformations?

In summary, canonical transformations do not change the volume in phase-space and Liouville's theorem states that the volume remains constant during motion. This means that every physical motion in phase-space can be described as a series of parametrized canonical transformations. However, these transformations only change the coordinate system, not the physical state of the system. For a Hamiltonian system, time evolution can be described as a canonical transformation with the Hamiltonian as the generator. This can be seen through the relationship between the time derivative of a phase-space function and the Hamiltonian function.
  • #1
Higgsono
93
4
When we make a canonical transformation the volume in phase-space doesn't change. Likewise if we consider motion of a system in phase-space the volume won't change either according to Liouville's theorem.

Does that mean that every physical motion of the system in phase-space is equivalent to some parametrization of a set of canonical transformations?
 
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  • #2
Yes and no.

No because the transformations change your coordinate system, not what physical state the system is in, whereas motion changes the state. Yes, because if you artificially kept the values of the coordinates constant, then yes you can come up with a series coordinate transforms which replicate the actual motion. It's the same mathematical machinery that let's you link together the rest frames of an accelerating observer via a one-parameter subgroup of Lorentz transformations and rotations.
 
  • #3
Yes, for a Hamiltonian system time evolution is a canonical transformation ("flow") with the Hamiltonian as generator. For any phase-space function ##f(q,p)## you have
$$\dot{f}=\{f,H \},$$
because
$$\dot{f}=\dot{q}^j \partial_{q^j} f+\dot{p}_j \partial_{p_j} f=\partial_{p_j} H \partial_{q^j} f - \partial_{q_j} H \partial_{p_j} f=\{f,H\}.$$
 

What are canonical transformations?

Canonical transformations are mathematical transformations that preserve the canonical form of Hamilton's equations in classical mechanics. They are used to transform a given set of coordinates and momenta into a new set, while preserving the underlying physics of a system.

Why are canonical transformations important?

Canonical transformations are important because they allow us to simplify the equations of motion and find new, more convenient coordinates and momenta for a given system. They also help us identify and understand the symmetries and conserved quantities of a system.

What are the two types of canonical transformations?

The two types of canonical transformations are point transformations and generating function transformations. Point transformations change the coordinates and momenta without introducing any new variables, while generating function transformations introduce new variables in the transformation process.

How do you determine if a transformation is canonical?

A transformation is canonical if it preserves the Poisson bracket structure of Hamilton's equations. This means that the Poisson bracket of any two functions in the original coordinates and momenta must be equal to the Poisson bracket of the corresponding transformed functions in the new coordinates and momenta.

What is the significance of the generating function in canonical transformations?

The generating function plays a crucial role in determining the new coordinates and momenta in a generating function transformation. It is a function of the old and new coordinates and momenta, and its partial derivatives with respect to the old coordinates and momenta give the new coordinates and momenta. It also helps us identify the type of transformation (e.g. point or generating function) and any symmetries in the system.

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