Abstract
The main distinction between the treatment of turbulent flow in this chapter and Chapter 7 and the treatment of laminar flows in Chapters 4 and 5 is that whereas the diffusivities of momentum and heat are known transport properties in laminar flow, the effective diffusivities in turbulent flow are not. Our knowledge of these turbulent diffusivities depends on measurements of flow characteristics such as mean velocity and temperature gradients, together with corresponding turbulent fluxes of momentum (the Reynolds stresses) and of heat, and is usually expressed in terms of empirically based models.
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Cebeci, T., Bradshaw, P. (1984). Uncoupled Turbulent Boundary Layers. In: Physical and Computational Aspects of Convective Heat Transfer. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02411-9_6
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DOI: https://doi.org/10.1007/978-3-662-02411-9_6
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