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Ground Boundary Conditions for Thermal Convection Over Horizontal Surfaces at High Rayleigh Numbers

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Abstract

We present “wall functions” for treating the ground boundary conditions in the computation of thermal convection over horizontal surfaces at high Rayleigh numbers using coarse numerical grids. The functions are formulated for an algebraic-flux model closed by transport equations for the turbulence kinetic energy, its dissipation rate and scalar variance, but could also be applied to other turbulence models. The three-equation algebraic-flux model, solved in a T-RANS mode (“Transient” Reynolds-averaged Navier–Stokes, based on triple decomposition), was shown earlier to reproduce well a number of generic buoyancy-driven flows over heated surfaces, albeit by integrating equations up to the wall. Here we show that by using a set of wall functions satisfactory results are found for the ensemble-averaged properties even on a very coarse computational grid. This is illustrated by the computations of the time evolution of a penetrative mixed layer and Rayleigh–Bénard (open-ended, 4:4:1 domain) convection, using \(10 \times 10 \times 100\) and \(10 \times 10 \times 20\) grids, compared also with finer grids (e.g. \(60 \times 60 \times 100\)), as well as with one-dimensional treatment using \(1 \times 1 \times 100\) and \(1 \times 1 \times 20\) nodes. The approach is deemed functional for simulations of a convective boundary layer and mesoscale atmospheric flows, and pollutant transport over realistic complex hilly terrain with heat islands, urban and natural canopies, for diurnal cycles, or subjected to other time and space variations in ground conditions and stratification.

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Notes

  1. The notion of unsteady Reynold-averaged Navier–Stokes (URANS) approach commonly implies the straightforward application of a RANS model in time-dependent mode to solve flows that are unsteady in the mean, and when the externally imposed time scale is much greater than the characteristic turbulence scale, justifying the use of the time-averaged equations. The URANS concept can also be applied to flows that can be regarded as steady in the mean, but inherently unsteady due to strong internal instabilities that generate quasi-periodic, deterministic turbulence structures, such as vortex shedding or convective cells in flows dominated by buoyancy or rotation. The T-RANS label is used for the latter to distinguish it from the common URANS applied to flows subjected to external mean flow unsteadiness.

  2. For convenience, in the following we deleted braces \(\langle {}\rangle \) for the resolved properties, as the analysis is applicable to general steady or unsteady RANS methods.

  3. Admittedly, using the well-resolved LES or DNS results would have been more appropriate for this exercise. However, detailed field data for the two cases considered (ensemble averaged wind velocity and temperature, friction velocity and heat flux along the wall, the reference near-wall point to define the characteristic turbulence velocity scale) are not readily available and would require laborious processing of the raw data. As the present analysis is more of a qualitative nature (collapsing of curves) and in view of the earlier satisfactory reproduction of LES by T-RANS, we opted for using the current dedicated T-RANS solutions.

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Acknowledgments

The work is supported by the Russian Science Fund, Grant No 14-29-00203_2014-16.

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Correspondence to M. Hrebtov.

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Hanjalić, K., Hrebtov, M. Ground Boundary Conditions for Thermal Convection Over Horizontal Surfaces at High Rayleigh Numbers. Boundary-Layer Meteorol 160, 41–61 (2016). https://doi.org/10.1007/s10546-016-0135-z

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