In this paper we derive upper bounds for the second order structure functio
n as well as for the Littlewood-Paley energy spectrum - an average of the u
sual energy spectrum E(k). While the upper bound results are consistent wit
h a Kolmogorov type dependence on wave number k, the bounds do not involve
the usual dissipation rate epsilon. Instead the bounds involve a dissipativ
e quantity <(epsilon)over cap> similar to epsilon but based on the L-3 aver
age of del u. Numerical computations for a highly symmetric flaws with Tayl
or microscale Reynolds numbers up to R-lambda = 155 are found to be consist
ent with the proposition that a relation in the inertial regime of the type
E(k) similar to (C) over cap<(epsilon)over cap>(2/3)k(-5/3) holds with con
stant (C) over cap. (C) 1999 American Institute of Physics. [S1070-6631(99)
00308-6].