Numerical and experimental results indicate that the critical amplitud
e for non-linear growth of disturbances in a uniform shear flow follow
s two scaling laws, depending on the shape of the initial disturbance:
i) a Re-1 law for disturbances with zero streamwise dependence (strea
ks) (Kreiss et al., submitted to J. Fluid Mech.); ii) a Re--0.4+/-0.1
law for disturbances with non-zero streamwise dependence (spots) (Dauc
hot and Daviaud, submitted to Phys. Fluid A). It is shown that these l
aws can be explained by the competition between non-linear growth and
viscous dissipation and that the difference in exponent simply reflect
s the difference in viscous-decay mechanism. Lower bounds for conditio
ns for non-linear growth are derived analytically. They follow a Re-1
and Re-1/3 law for streamwise and spotwise initial perturbations. The
transition to a self-sustained turbulent state is also discussed. Uppe
r bounds for this transition are derived. They follow, respectively, a
Re -1/2 and Re -1/6 law for streak or spot initial perturbations.