Abstract

The anomalous scaling exponents ζn\zeta_{n} of the longitudinal structure functions SnS_{n} for homogeneous isotropic turbulence are derived from the Navier-Stokes equations by using field theoretic methods to develop a low energy approximation in which the Kolmogorov theory is shown to act effectively as a mean field theory. The corrections to the Kolmogorov exponents are expressed in terms of the anomalous dimensions of the composite operators which occur in the definition of SnS_{n}. These are calculated from the anomalous scaling of the appropriate class of nonlinear Green's function, using an uvuv fixed point of the renormalisation group, which thereby establishes the connection with the dynamics of the turbulence. The main result is an algebraic expression for ζn\zeta_{n}, which contains no adjustable constants. It is valid at orders nn below % g_{\ast}^{-1}, where g∗g_{\ast} is the fixed point coupling constant. This expression is used to calculate ζn\zeta _{n} for orders in the range % n=2 to 10, and the results are shown to be in good agreement with experimental data, key examples being ζ2=0.7\zeta_{2}=0.7, ζ3=1\zeta_{3}=1 and % \zeta_{6}=1.8.Comment: REVTeX, 59 pages, icludes 8 .eps file

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    Last time updated on 27/02/2019