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Optimization and Computational Fluid Dynamics - Department of ...

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2 A Few Illustrative Examples <strong>of</strong> CFD-based <strong>Optimization</strong> 47<br />

100%<br />

80%<br />

60%<br />

40%<br />

20%<br />

0%<br />

0.10 [g/s]<br />

0.03 [g/s]<br />

1.6[g/s]<br />

0[g/s]<br />

10 × 10 −3 [g/s]<br />

6 × 10 −3 [g/s]<br />

20 [K]<br />

0[K]<br />

Methane Air CO Temp. variation<br />

Fig. 2.17 Input parameters <strong>and</strong> objectives <strong>of</strong> the EA optimization for good configurations<br />

in the laminar burner case<br />

they may fail or lead to inaccurate results. There are well-known issues like<br />

swirl, secondary flow, large pressure gradients, strong streamline curvature,<br />

etc., where model predictions <strong>of</strong>ten become poor. In such cases, some modifications<br />

<strong>and</strong>/or additional terms are needed in the model. Different authors<br />

<strong>of</strong>ten propose slightly different parameter values when introducing such modifications.<br />

The determination <strong>of</strong> the model constants for engineering turbulence models<br />

is indeed a difficult task. The values are <strong>of</strong>ten considered as some ad-hoc<br />

values. Changing one parameter in order to observe consequences concerning,<br />

for instance, the time-averaged turbulent velocity distribution or the<br />

shear-stress distribution is easy. But the simultaneous modification <strong>of</strong> several<br />

parameters <strong>of</strong> a turbulence model in order to increase accuracy rapidly becomes<br />

a formidable issue. If all the model parameters are changed in small<br />

steps, then the number <strong>of</strong> possible combinations would yield an enormous –<br />

<strong>and</strong> probably unnecessary – computational effort to explore the whole domain.<br />

In that case, numerical optimization techniques may help to speed-up<br />

the search procedure in order to find the best possible combination <strong>of</strong> the<br />

model constants with a minimum computational load, since optimization is<br />

much more efficient than a simple trial <strong>and</strong> error manual procedure.<br />

The objective in this case is to optimize the prediction <strong>of</strong> the time-averaged<br />

turbulent velocity distribution in channel flows. Direct numerical simulation<br />

(DNS) data [40, 60] for four different Reynolds numbers are chosen as ref-

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