Understanding the Concept of Canonical Transformation in Hamiltonian Mechanics

AI Thread Summary
The discussion centers on the concept of canonical transformations in Hamiltonian mechanics, specifically the independence of variables in the transformation from (q,p) to (Q,P). The confusion arises from the interpretation of q and Q as being separately independent, despite Q being a function of q. It is clarified that the independence refers to the absence of linear dependence between their time derivatives, which is crucial for preserving Hamilton's equations of motion. The relationship expressed through the time derivative of Q does not imply direct dependence, as it involves partial derivatives. Understanding this distinction is essential for grasping the underlying principles of canonical transformations.
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There's a part in my book that I don't understand. I have attached the part and it is basically about how to transform from a set of conjugate variables (q,p) to another (Q,P) while preserving the hamilton equations of motion. I don't understand what he means by q,Q being separately independent. Don't we seek transformation where Q is a function of q. Maybe I'm just not into what he means by this independency.
 

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It's true, but he means that for F q and Q are variables, so that there's no linear dependence between their time derivatives. Such a linear dependence would spoil his argument.
 
Please elaborate. If Q = Q(q,p,t) how is its time derivative independent of q? :(
 
Well, what is said was that there is no linear dependence between \displaystyle{\dot{Q}} and \displaystyle{\dot{q}}.
 
but dQ/dt = \partialQ/\partialq dq/dt + ...
How is that not a relation between them?
 
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