We construct an approximate renormalization scheme for Hamiltonian systems
with two degrees of freedom. This scheme is a combination of Kolmogorov-Arn
old-Moser (KAM) theory and renormalization-group techniques. It makes the c
onnection between the approximate renormalization procedure derived by Esca
nde and Doveil and a systematic expansion of the transformation. In particu
lar, we show that the two main approximations, consisting in keeping only t
he quadratic terms in the actions and the two main resonances, keep the ess
ential information on the threshold of the breakup of invariant tori.