Abstract
If the typical temperature difference in a gas flow is an appreciable fraction of the absolute temperature, the typical density difference will be an appreciable fraction of the absolute density, and the density appearing in the velocity-field equations can no longer be taken as constant. Instead, as in the buoyant flows of Chapter 9, the momentum and energy equations must be solved simultaneously since they are “coupled,” i.e., density appears in the momentum equation and is linked through an equation of state to the dependent variable of the energy equation.
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Cebeci, T., Bradshaw, P. (1984). Coupled Laminar Boundary Layers. In: Physical and Computational Aspects of Convective Heat Transfer. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02411-9_10
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DOI: https://doi.org/10.1007/978-3-662-02411-9_10
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