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Optimization and Computational Fluid Dynamics - Department of ...

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4 Adjoint Methods for Shape <strong>Optimization</strong> 101<br />

Absolute Gradient Value<br />

0.01<br />

0.0001<br />

1e-006<br />

1e-008<br />

1e-010<br />

1e-012<br />

1e-014<br />

1st cycle<br />

10th cycle<br />

converged<br />

1e-016<br />

1 2 3 4 5<br />

Design Variable<br />

(a)<br />

Hessian Value<br />

0.018<br />

0.016<br />

0.014<br />

0.012<br />

0.01<br />

0.008<br />

0.006<br />

0.004<br />

0.002<br />

0<br />

-0.002<br />

1st cycle<br />

10th cycle<br />

converged<br />

0 5 10 15 20 25<br />

Design Variable<br />

Fig. 4.4 Inverse design <strong>of</strong> a 2D duct (a) change in the objective function gradient values<br />

(absolute values) during the optimization (b) corresponding change in Hessian matrix<br />

values<br />

y<br />

0.1<br />

0.08<br />

0.06<br />

0.04<br />

0.02<br />

0<br />

0 0.5 1 1.5 2<br />

(a)<br />

x<br />

reference<br />

initial<br />

optimal<br />

Cp<br />

0.94<br />

0.93<br />

0.92<br />

0.91<br />

0.9<br />

0.89<br />

0.88<br />

0.87<br />

0.86<br />

0.85<br />

0.84<br />

(b)<br />

0 0.5 1 1.5 2<br />

(b)<br />

x<br />

reference<br />

initial<br />

optimal<br />

Fig. 4.5 Inverse design <strong>of</strong> a 2D duct (a) comparison <strong>of</strong> the initial, optimal <strong>and</strong> reference<br />

airfoil contours (not in scale) (b) comparison <strong>of</strong> the initial, optimal <strong>and</strong> target pressure<br />

distributions<br />

also shown. This curve quantifies the difference (absolute value) in the actual<br />

blade airfoil thickness, at specific chord-wise positions, from the corresponding<br />

minimum allowed ones. The latter are defined to be equal to the 90% <strong>of</strong><br />

an existing (reference) airfoil. If any <strong>of</strong> these local constraints are violated,<br />

a penalty value is added to the total penalty value. So, zero penalty values<br />

correspond to a non-violated thickness constraint. During the first five cycles,<br />

losses are reduced almost by 1.5%, while none <strong>of</strong> the thickness constraints are<br />

violated. The reduction rate in total pressure losses decreased during the subsequent<br />

cycles <strong>and</strong> oscillations became apparent due to occasional constraint<br />

violations. Upon convergence (for which around 40 cycles are needed), the<br />

thickness constraints are not violated any more or are just slightly violated.<br />

The reduction rate <strong>of</strong> the gradient values for all design variables are shown<br />

in Fig. 4.8. The objective function gradient with respect to the suction side

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