The major difficulty in developing theories for anomalous scaling in hydrod
ynamic turbulence is the lack of a small parameter. In this letter we intro
duce a shell model of turbulence that exhibits anomalous scaling with a tun
able parameter epsilon, 0 less than or equal to epsilon less than or equal
to 1, representing the ratio between deterministic and random components in
the coupling between N identical copies of the turbulent field. Our numeri
cal experiments give strong evidence that in the limit N --> infinity anoma
lous scaling sets in proportional to epsilon(4) This result shows consisten
cy with the nonperturbative closure proposed by the authors in Phys. Fluids
, 12 (2000) 803. In this procedure closed equations of motion for the low-o
rder correlation and response functions are obtained, keeping terms proport
ional to epsilon(0) and epsilon(4), discarding terms of orders epsilon(6) a
nd higher. Moreover we give strong evidences that the birth of anomalous sc
aling appears at a finite critical epsilon, being epsilon(c) approximate to
0.6.