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Optimization and Computational Fluid Dynamics - Department of ...

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4 Adjoint Methods for Shape <strong>Optimization</strong> 103<br />

Gradient<br />

1.8<br />

1.6<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

-0.2<br />

0 5 10 15 20 25<br />

(a)<br />

Variable<br />

Gradient<br />

1.8<br />

1.6<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

-0.2<br />

0 5 10 15 20 25<br />

(b)<br />

Variable<br />

initial<br />

optimal<br />

Fig. 4.8 Total pressure losses minimization in a 2D compressor cascade (a) convergence<br />

history <strong>of</strong> the objective function gradient values <strong>and</strong> (b) gradient values for the initial <strong>and</strong><br />

optimal cascade airfoils<br />

y<br />

0.16<br />

0.14<br />

0.12<br />

0.1<br />

0.08<br />

0.06<br />

0.04<br />

0.02<br />

0<br />

-0.02<br />

0 0.2 0.4 0.6 0.8 1<br />

(a)<br />

x<br />

initial<br />

optimal<br />

y<br />

0.5<br />

0.45<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

-0.05<br />

-0.1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9<br />

(b)<br />

x<br />

initial<br />

optimal<br />

Fig. 4.9 Total pressure losses minimization in a 2D compressor cascade (a) initial <strong>and</strong><br />

optimal set <strong>of</strong> Bézier control points <strong>and</strong> (b) the corresponding cascade airfoil contours<br />

corrected gradient values “push” both suction <strong>and</strong> pressure side control points<br />

away from each other.<br />

Improvements in aerodynamic characteristics are shown in Figs. 4.10 <strong>and</strong><br />

4.11 where the initial <strong>and</strong> optimal pressure <strong>and</strong> friction coefficients are shown.<br />

A close-up view <strong>of</strong> the flow developed close to the trailing edge over the suction<br />

side is shown. Both figures show that separation on the optimal blade airfoil<br />

is kept minimum or even disappears. The static pressure plateau <strong>and</strong> the<br />

negative friction coefficient values are significantly reduced. The improvement<br />

<strong>of</strong> separation is also shown in Fig. 4.12 where the Mach number distribution<br />

is shown for the initial <strong>and</strong> optimal configuration.<br />

Similar results can be obtained using the entropy generation instead <strong>of</strong><br />

the total pressure loss as objective function [52, 53]. These are omitted in the<br />

interest <strong>of</strong> space.

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