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Numerical Study of Passive and Active Flow Separation Control ...

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airfoil is shown in Fig. 14. The negative value <strong>of</strong> C between x = 0.06C <strong>and</strong> x = 0.285C,<br />

f<br />

indicates the near-wall reversed flow in the separation bubble. Both Fig. 13 <strong>and</strong> Fig. 14<br />

confirm the observation in Fig. 11 <strong>and</strong> Fig. 12 in terms <strong>of</strong> the location <strong>and</strong> length <strong>of</strong> the<br />

separation bubble. The abrupt recovery <strong>of</strong> C from its negative peak to a positive peak<br />

f<br />

between x = 0.25C <strong>and</strong> x = 0.35C corresponds to transition <strong>and</strong> reattachment <strong>of</strong> the<br />

separated flow.<br />

Fig. 13. Mean pressure coefficient <strong>of</strong><br />

baseline case<br />

18<br />

Fig. 14. Mean skin friction coefficient <strong>of</strong><br />

baseline case<br />

The chord-wise distribution <strong>of</strong> peak turbulence kinetic energy k is displayed in Fig.<br />

15. The ‘peak’ means the maximum k at each streamwise location. The abrupt increase <strong>of</strong><br />

k at xº 0.24C indicates the starting point <strong>of</strong> transition to turbulence, which is also shown<br />

by the sharp increase <strong>of</strong> C displayed in Fig. 14. It is clear that transition occurs before<br />

f<br />

the separated flows reattaches, because the mean reattachment point is at x = 0.285C<br />

while transition starts at x º 0.24C.

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