Tuesday, November 3, 2015

homework and exercises - A problem with canonical transformation exchanging p and q


Any function F of the old coordinate q and the new coordinate Q describes the canonical transformation according to pdqPdQ=dF(q,Q)

where p,P are the old and new momentums respectively. From this relation follows p=Fq,P=FQ
Also, defining Φ=F+PQ one has pdq+QdP=dΦ
and hence Φ is naturally a function of q,P. Relation (2) implies that p=Φq,Q=ΦP
I want to check formulas (1) and (3) at an explicit example. Let us choose F=qQ. Then from (1) follows p=Q,P=q
That is indeed a canonical transformation exchanging (p,q)(Q,P). My problem is with formula (3). In fact, Φ=F+PQ=(q+P)Q=0
since P=q. Naively then (3) implies that p=Q=0. What is the trap that I've fallen into?



Answer





  1. Let us here for simplicity only discuss 2D phase spaces. Then a CT carves out a codimension-2 (or 3D) submanifold in the 5D space M with local coordinates (q,p,Q,P,t).




  2. OP's trap seems to be to think that any CT can be reproduced with all of the four type 1-4 generating functions. Locally it is generically true, but there are counterexamples, such as, e.g. OP's CT (Q,P) = (p,q).

    The good news is that (one may show that) for any CT at least one of the type 1-4 generating functions works locally.





  3. Let us note for later that the codimension-2 submanifold in OP's case (A) is determined by the 2 conditions (A).




  4. The CT (A) works nicely with a type 1 generating function F(q,Q,t)=qQ, as OP already noted.




  5. However, there is no type 2 generating function Φ(q,P,t). The problem is that the type 2 CT is a graph from the 3D space with coordinates (q,P,t) to M, which can never reproduce OP's CT (A). [The variables q & P are independent in a type 2 graph, but constrained to be opposite in the CT (A).]





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