Prediction of the near wall region is crucial to the accuracy of turbulent flow computational fluid dynamics (CFD) simulation. However, sufficient near-wall resolution is often prohibitive for high Reynolds number flows with complex geometries, due to high memory and processing requirements. A common approach in these cases is to use wall functions to bridge the region from the first grid node to the wall. This paper presents an alternative method that relaxes the near wall resolution requirement by solving one dimensional transport equations for velocity and turbulent kinetic energy across a locally defined subgrid contained within wall adjacent grid cells. The addition of the subgrid allows for wall adjacent primary grid sizes to vary arbitrarily from low-Re model sizing (y+≈1) to wall function sizing without significant loss of accuracy or increase in computational cost. The method is applied to zero pressure gradient flow over a flat plate and yields solutions comparable to low-Re modeling with high near-wall resolution. Unlike low-Re or wall function modeling, the new method is shown to be insensitive to size variations of the first primary grid cell.

1.
Patankar, S. V., and Spalding, D. B., 1967, Heat and Mass Transfer in Boundary Layers, Morgan-Grampian Press, London.
2.
Launder
B. E.
, and
Spalding
D. B.
,
1974
, “
The Numerical Computation of Turbulent Flows
,”
Computer Methods in Applied Mechanics and Engineering
,
3
, pp.
269
289
.
3.
Chieng
C. C.
, and
Launder
B. E.
,
1980
, “
On the Calculation of Turbulent Heat Transport Downstream from an Abrupt Pipe Expansion
,”
Numerical Heat Transfer
,
3
, pp.
189
207
.
4.
Amano
R. S.
,
1984
, “
Development of a Turbulence Near-Wall Model and Its Application to Separated and Reattached Flows
,”
Numerical Heat Transfer
,
7
, pp.
59
75
.
5.
Ciofalo
M.
, and
Collins
M. W.
,
1989
, “
k-e Predictions of Heat Transfer in Turbulent Recirculating Flows Using an Improved Wall Treatment
,”
Numerical Heat Transfer Part B: Fundamentals
,
15
, pp.
21
47
.
6.
Kim, S.-E., and Choudhury, D., 1995, “A Near-Wall Treatment Using Wall Functions Sensitized to Pressure Gradient,” ASME FED, 217, Separated and Complex Flows.
7.
Shih, T.-H., Povinelli, L. A., and Liu, N.-S., 2003, “Application of Generalized Wall Function for Complex Turbulent Flows,” Journal of Turbulence, 4, No. 015.
8.
Nichols
R. H.
, and
Nelson
C. C.
,
2004
, “
Wall Function Boundary Conditions Including Heat Transfer and Compressibility
,”
AIAA Journal
,
42
, pp.
1107
1114
.
9.
Kalitzin
G.
,
Medic
G.
,
Iaccarino
G.
, and
Durbin
P. A.
,
2005
, “
Near-Wall Behavior of RANS Turbulence Models and Implications for Wall Function
,”
Journal of Computational Physics
,
204
, pp.
265
291
.
10.
Craft
T. J.
,
Gant
S. E.
,
Iacovides
H.
, and
Launder
B. E.
,
2004
, “
A New Wall Function Strategy for Complex Turbulent Flows
,”
Numerical Heat Transfer Part B: Fundamentals
,
45
, pp.
301
318
.
11.
Wolfshtein
M.
,
1969
, “
The Velocity and Temperature Distribution of One-Dimensional Flow with Turbulence Augmentation and Pressure Gradient
,”
International Journal of Heat and Mass Transfer
,
12
, pp.
301
318
.
This content is only available via PDF.
You do not currently have access to this content.