Find the projections on the phase planes of the phase space motion of a two-dimensional harmonic oscillator.
In Cartesian coordinates,
H=2m1(px2+py2)+2kxx2+2kyy2 (9.114)
and the Hamilton-Jacobi equation (9.54) is separable in the form W(x, y) = W1(x) +W2(y) where
H=(q1,...,qn,∂q1∂W,...,∂qn∂W)=α1. (9.54)
2m1(dxdW1)2+2kxx2=αx, (9.115a)
2m1(dydW2)2+2kyy2=αy, (9.115b)
with
H=α1=αx+αy. (9.116)
Since px=dW1/dx and py=dW2/dy, Eqs. (9.115) represent ellipses on the phase planes (x, px) and (y, py), respectively. Although both projections are periodic with periods τx=2π/ωx=2π(m/kx)1/2 and τy=2π/ωy=2π(m/ky)1/2, the motion in phase space will only be periodic if the frequencies ωx and ωy are commensurate – that is, if ωx/ωy is a rational number. Indeed, if τ is the period of the motion, the phase space path closes in the course of the time interval τ .The projections also close, so τ has to be an integer number of periods τx and τy – that is, there exist integers m and n such that τ=m2π/ωx=n2π/ωy, whence ωx/ωy=m/n is a rational number.