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Table 2-5 Summary of Approaches to Turbulence Modelinga Model Boussinesq approximation One equation with one adjustable parameter Averaged over time and all length scales Prandtl mixing length One equation with two adjustable parameters Averaged over time and all length scales Physical Basis of the Model One length scale Based on analogy to laminar transport and apparent viscosity One length scale Based on analogy to mean free path in the kinetic theory of gases Drawbacks Oversimpli cation of the physics The apparent viscosity is a function of the ow eld and of position Oversimpli cation of the physics The assumption of a linear velocity pro le does not match physical reality; however, the results are surprisingly good for the log-law region of a pipe Five model constants have been determined for simpli ed ows Two-equation models cannot accurately model the effects of anisotropy on the large scale, although the form of the model may be useful for the locally isotropic range of turbulence k model tends to be overly diffusive datamatrix.net example DataMatrix . NET Control C# Tutorial | DataMatrix Barcode | Barcode ...
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