mjordan2nd
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Homework Statement
Let Q^1 = (q^1)^2, Q^2 = q^1+q^2, P_{\alpha} = P_{\alpha}\left(q,p \right), \alpha = 1,2 be a CT in two freedoms. (a) Complete the transformation by finding the most general expression for the P_{\alpha}. (b) Find a particular choice for the P_{\alpha} that will reduce the Hamiltonian
H = \left( \frac{p_1 - p_2}{2q^1} \right)^2 + p_2 + (q^1 + q^2)^2
to
K = P_1^2 + P_2.
Homework Equations
The Attempt at a Solution
I have shown that
P_1 = \frac{1}{2q^1} \left( p_1 + \frac{\partial F}{\partial q^1} - p_2 - \frac{\partial F}{\partial q^2} \right),
P_2 = p_2 + \frac{\partial F}{\partial q^2}
is the most general canonical transformation for the momenta, where F=F(q^1, q^2). This is consistent with the solution manual. For part b, however, the answer I get for an intermediate step is inconsistent with the solutions manual, and I don't understand why. Given that the transformation is canonical, all I need to do to find the transformed Hamiltonian K is find the inverse transformation and plug it into the Hamiltonian H. The inverse transformation is
p_2 = P_2 - \frac{\partial F}{\partial q^2},
p_1 = 2q^1P_1 + P_2 - \frac{\partial F}{\partial q^1}.
Plugging this into H, and renaming H to K since it's in terms of the transformed coordinates we have
K = P_1^2 + P_2 - \frac{\partial F}{\partial q^2} + (q^1 + q^2)^2.
Since we want K to be
K = P_1^2 + P_2,
this means
\frac{\partial F}{\partial q^2} = (q^1+q^2)^2 = (q^1)^2+(q^2)^2+2q^1q^2.
F=q^2(q^1)^2 + \frac{1}{3}(q^2)^3 +q^1(q^2)^2 + C.
Plugging this into the general transformation I derived I find that
P_1 = \frac{1}{2q^1} \left(p_1-p_2-(q^1)^2 \right),
P_2 = (q^1+q^2)^2+p_2.
My equation for P_2 is consistent with the solutions manual, but my equation for P_1 is not. According to the solutions manual
P_1=\frac{p_1+p_2}{2q^1}.
So my question is, where did I go wrong. I have worked out the problem twice, and get the same answer for P_1.
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