The first Hopf bifurcation of the infinite cylinder wake is analysed t
heoretically and by direct simulation. It is shown that a decompositio
n into a series of harmonics is a convenient theoretical and practical
tool for this investigation. Two basic properties of the instability
allowing the use and truncation of the series of harmonics are identif
ied: the lock-in of frequencies in the flow and separation of the rapi
d timescale of the periodicity from the slow timescale of the non-peri
odic behaviour. The Landau model is investigated under weak assumption
s allowing strong nonlinearities and transition to saturation of ampli
tudes. It is found to be rather well satisfied locally at a fixed posi
tion of the flow until saturation. It is shown, however, that no trunc
ated expansion into a series of powers of amplitude can account correc
tly for this fact. The validity of the local Landau model is found to
be related to the variation of the form of the unstable mode substanti
ally slower than its amplification. Physically relevant characteristic
s of the Hopf bifurcation under the assumption of separation of three
timescales - those of the periodicity, amplification and deformation o
f the mode - are suggested.