Diapycnal eddy diffusivity: Difference between revisions

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Osborn 1980 showed that <math>K_\rho =\frac{\bar{w'\rho'}}{\partial \rho/\partial z}\Gamma \epsilon N^{-2}</math>
Osborn 1980<ref>Osborn, T. R. (1980). Estimates of the Local Rate of Vertical Diffusion from Dissipation Measurements, Journal of Physical Oceanography, 10(1), 83-89</ref> showed that the buoyancy eddy diffusivity <math>K_\rho =\frac{\bar{w'\rho'}}{\partial \rho/\partial z}</math> could be reduced to  <math>K_\rho=\Gamma \epsilon N^{-2}</math> via the "mixing efficiency" <math>\Gamma</math> and the background stratification <math>N=\sqrt{\frac{-g}{\rho_o}\frac{\partial\rho}{\partial z}}</math>.

Latest revision as of 14:59, 22 April 2022


Short definition of Diapycnal eddy diffusivity (Diapycnal eddy diffusivity Kρ)
Diapycnal eddy diffusivity (for buoyancy) is defined from the buoyancy flux wρ and the background density gradient ρz

This is the common definition for Diapycnal eddy diffusivity, but other definitions maybe discussed within the wiki.

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Osborn 1980[1] showed that the buoyancy eddy diffusivity Kρ=wρ¯ρ/z could be reduced to Kρ=ΓϵN2 via the "mixing efficiency" Γ and the background stratification N=gρoρz.

  1. Osborn, T. R. (1980). Estimates of the Local Rate of Vertical Diffusion from Dissipation Measurements, Journal of Physical Oceanography, 10(1), 83-89