Order of steps on Hamiltonian canonical transformations

In summary, when performing a canonical transformation and finding the new Hamiltonian using K = H +\frac{\partial G}{\partial t}, the generating function must be of the form G(q,P,t). The partial derivative with respect to t would be taken while holding q and P constant, and then substituted for the new coordinates Q and P.
  • #1
carllacan
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Just a little doubt.

When we are performing a canonical transformation on a Hamiltonian and we have the equations of the new coordinates in terms of the old ones we have to find the Kamiltonian/new Hamiltonian using [itex]K = H +\frac{\partial G}{\partial t}[/itex]. My question is: do we have to derive the generating function before or after substituting the old coordinates for the new ones?

For example, in a [itex](q, p)\rightarrow(Q, P)[/itex] that last derivative would be [itex]\frac{\partial G(q, p, t)}{\partial t}[/itex] or [itex]\frac{\partial G(q(Q, P, t), p(Q, P, t))}{\partial t} =\frac{\partial G(Q, P, t}{\partial t}[/itex]?
 
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  • #2
carllacan said:
Just a little doubt.

When we are performing a canonical transformation on a Hamiltonian and we have the equations of the new coordinates in terms of the old ones we have to find the Kamiltonian/new Hamiltonian using [itex]K = H +\frac{\partial G}{\partial t}[/itex]. My question is: do we have to derive the generating function before or after substituting the old coordinates for the new ones?

For example, in a [itex](q, p)\rightarrow(Q, P)[/itex] that last derivative would be [itex]\frac{\partial G(q, p, t)}{\partial t}[/itex] or [itex]\frac{\partial G(q(Q, P, t), p(Q, P, t))}{\partial t} =\frac{\partial G(Q, P, t}{\partial t}[/itex]?

The generating function is always a function of both old and new coordinates. So it would not be of the form ##G(q,p,t)## since that would be a function of only the old coordinates.

There are four possible forms: ##G(q,Q,t)##, ##G(q,P,t)##, ##G(p,Q,t)##, and ##G(p,P,t)##.

Suppose you have the form ##G(q,P,t)##. Then ##q## and ##P## would be considered independent variables in ##G##.

When taking the partial derivative ##\frac{\partial G(q,P,t)}{\partial t}## you would hold ##q## and ##P## constant while taking the derivative with resepct to ##t##.

Afterwards you could substitute for q in terms of ##Q## and ##P## in order to express ##\frac{\partial G(q,P,t)}{\partial t}## in terms of the new coordinates.
 
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FAQ: Order of steps on Hamiltonian canonical transformations

1. What is a Hamiltonian canonical transformation?

A Hamiltonian canonical transformation is a mathematical process that changes the variables used to describe the state of a physical system while preserving the fundamental equations of motion. It is used in classical mechanics to simplify the equations of motion and make them more easily solvable.

2. What are the steps involved in a Hamiltonian canonical transformation?

The steps involved in a Hamiltonian canonical transformation are:

  • Identify the initial set of variables (known as the "old variables") used to describe the system.
  • Choose a new set of variables (known as the "new variables") that will make the equations of motion simpler.
  • Construct a generating function that relates the old and new variables.
  • Use this generating function to transform the Hamiltonian and the canonical equations of motion into the new variables.
  • Verify that the new set of equations is equivalent to the old ones.

3. Why are Hamiltonian canonical transformations important?

Hamiltonian canonical transformations are important because they allow us to simplify the equations of motion and make them easier to solve. They also provide a way to express the same physical system in different sets of coordinates, which can be useful in analyzing and understanding the system.

4. What is the difference between a canonical transformation and a Hamiltonian canonical transformation?

A canonical transformation is a more general mathematical process that preserves the form of Hamilton's equations, while a Hamiltonian canonical transformation specifically preserves the Hamiltonian function and the canonical equations of motion. In other words, all Hamiltonian canonical transformations are canonical transformations, but not all canonical transformations are Hamiltonian canonical transformations.

5. Can a Hamiltonian canonical transformation change the physical properties of a system?

No, a Hamiltonian canonical transformation does not change the physical properties of a system. It only changes the way in which those properties are described and calculated. The underlying physical system remains the same.

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