Question about canonical transformations

In summary, the author has a problem with calculating a canonical transformation, and doesn't know what an "associated canonical transformation" is.
  • #1
javiergra24
19
0
Hi everybody

I've got a problem related to canonical transformations that I can`t solve:

Given the expression of the canonical transformation

[tex]
Q=3q\cdot\big[ \exp\big((p+q)^5\big)+1\big] +3p\cdot \big[\exp((p+q)^5)+1\big]+p
[/tex]
[tex]
P=p+q
[/tex]
I have to calculate an associated canonical transformation. Anybody can help me?

Thanks
 
Physics news on Phys.org
  • #2
Are you sure you have stated exactly your problem?
 
  • #3
Exact problems is (from exam):
Given the transformation

[tex]
Q=3q\cdot\big[ \exp\big((p+q)^5\big)+1\big] +p\cdot \big[2\exp((p+q)^5)-1\big]
[/tex]

[tex]
P=q+p
[/tex]

Modify it slightly in order to be canonical

Answer. After imposing the condition for the Poisson bracket (equal to one) we get the result:
[tex]
\boxed{Q=3q\cdot\big[ \exp\big((p+q)^5\big)+1\big] +3p\cdot \big[\exp((p+q)^5)+1\big]+p}
[/tex]

In part two we're asked to obtain an associated canonical transformation. But after reading my books and papers about mechanics I still don't know what's an "associated trasformation mean". Is it the inverse transformation?
 
Last edited:
  • #4
OK. Now part of the problem is clear - supposing it is indeed a canonical transformation (I didn't check). But what the author of this exercise means by an "associated canonical transformation" - that I don't know.
 
  • #5
arkajad said:
OK. Now part of the problem is clear - supposing it is indeed a canonical transformation (I didn't check). But what the author of this exercise means by an "associated canonical transformation" - that I don't know.

Same here. I suppose the questioner might just be looking for an equivalent transformation, but written in a different functional form... something like

[tex]Q=Q(q,P)=3P\left(e^{P^5}+1\right) +P-q[/tex] and [tex]P=q+p[/tex]
instead of
[tex]Q=Q(q,p)=3q\left(e^{(p+q)^5}+1\right)+3p\left(e^{(p+q)^5}+1\right)+p[/tex] and [tex]P=q+p[/tex]

...but that's just a guess
 

FAQ: Question about canonical transformations

What is a canonical transformation?

A canonical transformation is a mathematical transformation that preserves the canonical form of the equations of motion in classical mechanics. It is a change of coordinates that does not change the physical properties or dynamics of the system.

What is the purpose of a canonical transformation?

The purpose of a canonical transformation is to simplify the equations of motion for a system by transforming the coordinates in a way that makes the problem easier to solve. It can also reveal hidden symmetries or conserved quantities of the system.

3. What are the conditions for a transformation to be canonical?

In order for a transformation to be canonical, it must satisfy two conditions: 1) it must preserve the form of Hamilton's equations, and 2) it must preserve the Poisson bracket relationships between the canonical coordinates and momenta.

4. How is a canonical transformation different from a regular coordinate transformation?

A canonical transformation is different from a regular coordinate transformation in that it preserves the equations of motion and the Poisson bracket relationships, whereas a regular coordinate transformation may change the form of these relationships. Additionally, a canonical transformation is usually used to simplify the equations of motion, while a regular coordinate transformation may be used for other purposes such as changing the coordinate system to one that is more convenient for a specific problem.

5. What are some examples of canonical transformations?

Some examples of canonical transformations include translation, rotation, and scaling transformations in classical mechanics. In quantum mechanics, the unitary transformation used to change between different bases is a canonical transformation. Other examples include the Legendre transformation used to transform between the Lagrangian and Hamiltonian formalisms, and the canonical transformation used to transform between different sets of generalized coordinates and momenta in Hamiltonian mechanics.

Back
Top