Find the canonical transformation generated by
F1(q,Q,t)=2tm(q−Q)2 (8.26)
and apply it to solving the problem of the motion of a one-dimensional free particle, whose Hamiltonian is H = p²/2m.
From Eqs. (8.9) we have
pi=∂qi∂F1,Pi=−∂Qi∂F1, i=1,...,n (8.9)
p=∂q∂F1=tm(q−Q), P=−∂Q∂F1=tm(q−Q), (8.27)
or, in direct form,
Q = q −mpt, P = p . (8.28)
On the other hand,
K(Q, P, t) = H(q, p, t) + ∂t∂F1=2mp2−2t2m(q−Q)2=2mP2−2mP2=0. (8.29)
The new Hamiltonian is identically zero and the transformed Hamilton’s equations are trivially solved:
Q˙=∂P∂K=0⟹ Q=a,P˙=−∂Q∂K=0⟹ P=b, (8.30)
where a and b are arbitrary constants. Returning to the original variables we finally obtain
q=a+mbt, (8.31)
which is the general solution to the equation of motion for the free particle.