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Optimization and Computational Fluid Dynamics - Department of ...

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50 Gábor Janiga<br />

The modified k–ω turbulence model proposed by Wilcox [79] in 1998 is<br />

employed in this study. The transport equations for k <strong>and</strong> ω can be written<br />

as, respectively:<br />

∂k<br />

∂t<br />

∂ω<br />

∂t<br />

∂k<br />

+ Uj<br />

∂xj<br />

∂ω<br />

+ Uj = α<br />

∂xj<br />

ω<br />

∂Ui<br />

= τij − β<br />

∂xj<br />

∗ kω + ∂<br />

�<br />

(ν + σ<br />

∂xj<br />

∗ νT) ∂k<br />

�<br />

∂xj<br />

k τij<br />

∂Ui<br />

− βω<br />

∂xj<br />

2 + ∂<br />

∂xj<br />

�<br />

(ν + σνT) ∂ω<br />

∂xj<br />

�<br />

, (2.18)<br />

. (2.19)<br />

The model includes several auxiliary relations <strong>and</strong> closure coefficients 1 .In<br />

this study, five parameters <strong>of</strong> the model are selected for the optimization,<br />

listed here with their st<strong>and</strong>ard values:<br />

α =13/25 ,β0 =9/125 ,β ∗ 0 =9/100 ,σ=1/2 ,σ∗ =1/2 . (2.20)<br />

A more detailed description <strong>of</strong> this turbulence model as well as the extension<br />

<strong>of</strong> this model to compressible flows is extensively discussed in Wilcox [79].<br />

2.5.2 Numerical Results<br />

After calculating one set <strong>of</strong> values for the four selected Reynolds numbers, the<br />

time-averaged turbulent velocity pr<strong>of</strong>iles are compared with the DNS results.<br />

The differences between the four corresponding pr<strong>of</strong>iles are measured using<br />

the area enclosing the curves. Due to the fine grid, this area can be approximated<br />

quite well using a simple numerical integration based on the rectangle<br />

rule. The four corresponding numerical parameters to optimize (minimize)<br />

are these area values for the four different Reynolds numbers.<br />

The main drawback associated to EAs in general remains their cost in<br />

terms <strong>of</strong> computing time because they require a large number <strong>of</strong> evaluations<br />

on different configurations. Here, a fast computational procedure is chosen in<br />

this investigation to speed-up the optimization. The numerical simulations<br />

for a fully developed channel flow are performed using the simplified computational<br />

code from Wilcox [79]. This program is based on a simple numerical<br />

integration <strong>and</strong> one single simulation takes only a few seconds on a st<strong>and</strong>ard<br />

PC.<br />

Five values have been selected as the input parameters <strong>of</strong> the optimization<br />

procedure. The model parameters α, β0, β ∗ 0 , σ <strong>and</strong> σ∗ mayfreelyvary<br />

between 0 <strong>and</strong> 1. A graphical representation in five dimensions is difficult.<br />

Therefore, parallel coordinates are used to show the connection between the<br />

1 In this work, these closure coefficients are referred to as model parameters. Calling them<br />

“model constant” is confusing, since these values are probably not constant <strong>and</strong> possibly<br />

problem-dependent.

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