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Hybrid wall functions: a step toward simplifying wall treatment

Julien de Charentenay, STAR-CD Developer, CD-adapco

 
 

We have implemented a new treatment of near-wall boundary conditions, developed by T. Rung [1], that removes constraints on near wall mesh density. This "hybrid wall function" treatment allows more accurate solutions to be obtained when the near-wall mesh is not optimized. If the mesh is fine enough, the boundary layer is resolved in a similar way to a low Reynolds number turbulence model. When the near-wall cell is located in the fully developed part of the boundary layer, adequate wall functions are applied. This boundary condition is available for the following turbulence models: k-epsilon linear/cubic/quadratic, k-omega standard and SST; with heat and mass transfer.

 
   
 

Fig. 1 presents a simulation of flow over a hill. The wall distance of the near-wall cell is constant along the bottom wall. However, the normalized wall distance y+, shown in Fig. 1, varies from 1 to 40 due to changes in flow velocity. Therefore, the mesh is not optimized for either low-Reynolds or high-Reynolds number turbulence models. However, using a linear k-epsilon turbulence model with the hybrid wall function, the agreement between predicted and measured flow field is excellent, as shown in Fig. 2.

Velocity vectors for the simulation of the turbulent flow and heat transfer in a cavity are presented in Fig. 3. The inlet flow corresponds to a fully developed boundary layer and can be accurately modeled using a coarse mesh and wall functions. However, a large re-circulation zone forms in the cavity. In this region, the flow velocity is small and the boundary layer must be resolved to accurately predict heat transfer. Using the hybrid wall function, the wall treatment automatically adapts to the near-wall mesh density and the flow field is accurately predicted with a limited number of cells. For this configuration, the predicted Nusselt number on the bottom wall of the cavity agrees well with experimental measurements, as shown in Fig. 4.

Fig. 5 shows the normalized wall distance at wall boundaries for a HVAC geometry provided by BEHR. The hybrid wall function has been successfully applied to this test-case and a 5% difference in pressure drop between inlet and outlet has been observed compared to the high-Reynolds number turbulence model.

[1] T. Rung. Formulierung universeller Wandrandbedingungen fur Transportgleichungsturbulenzmodelle. Technische Universitat Berlin. Institutsbericht Nr. 02/99



Fig. 5: Normalized wall distance y+ (scale from 0 to 100) for a HVAC system. Courtesy of BEHR


Fig. 1: Isocontours of velocity magnitude and normalized wall distance y+ (scale from 0 to 40) at the lower wall for flow over a hill



Fig. 2: Comparison of stream-velocity profile at two different sections for flow over a hill



Fig. 3: Velocity vectors and Nusselt number on the cavity wall for flow in a cavity



Fig. 4: Comparison of predicted and measured Nusselt numbers on the cavity wall

 
     
 
 
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