The deviations deltazeta(m) (''intermittency corrections'') from class
ical (''K41'') scaling zeta(m)=m/3 of the mth moments [\u(p)\m] in hig
h Reynolds number turbulence are calculated, extending a method to app
roximately solve the Navier-Stokes equation described earlier. It is s
uggested to introduce the notion of scale resolved intermittency corre
ctions deltazeta(m)(p), because these deltazeta(m)(p) are found to be
large in the viscous subrange, moderate in the nonuniversal stirring s
ubrange but, surprisingly, extremely small if not zero in the inertial
subrange. If ISR intermittency corrections persisted in experiment up
to the large Reynolds number limit, it would show by calculation that
this could be due to the opening of phase space for larger wave vecto
rs. In the higher order velocity moments [\u(p)\m] the crossover betwe
en inertial and viscous subrange is (10etam/2)-1, thus the inertial su
brange is smaller for higher order moments.