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Astron. Astrophys. 351, 347-358 (1999) Appendix A: derivation of the Eq. 38The diffusion coefficient as functions of the variables in Fourier space is: The Fourier transform is given by the following expression: (with The velocity can be expressed with the inverse Fourier transform: as well as the partial derivative of the velocity: where the monochromatic component
We therefore have the expression of the vertical diffusion coefficient: From now on This implies the presence of three products, but the integral taken over two of them does vanish. Therefore, the ensemble average of the four terms in Eq. (37) can be obtained as the product of two ensemble averages: The first ensamble average is given by the following equation: with the term between brackets tends to
So, and where from Lesieur (V-5-4): and the mean square velocity for 3D and 2D turbulence is given by: Furthermore, for the dependence on frequency of the turbulence spectrum, we chose an exponentiel one: and, So, the expression from Lessieur (p.111), for 3D case,
which leads to a new expression of
From Eq. (A8) and Eq. (A10) we hve a new expression of the diffusion coefficient: Introducing a new variable with ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1999 Online publication: November 2, 1999 ![]() |