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The significance of coherent flow structures for the turbulent mixing ...

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6 Investigation <strong>of</strong> <strong>the</strong> xz-plane<br />

300<br />

250<br />

z<br />

+<br />

200<br />

150<br />

Q4<br />

Q4<br />

Q4<br />

Q4<br />

100<br />

50<br />

300<br />

0<br />

0 50 100 150 200 250 300 350 400 450 500 550<br />

250<br />

??]<br />

x [???]<br />

200<br />

z<br />

+<br />

150<br />

100<br />

50<br />

0<br />

0 50 100 150 200 250 300 350 400 450 500 550<br />

FIGURE 6.26: Velocity fluctuations measured simultaneously at Ó ® Ú¥Ø<br />

(top) and Ó ® óÜ Ø<br />

.<br />

x<br />

+<br />

??]<br />

x [???]<br />

effect, <strong>the</strong> streaks move away from <strong>the</strong> wall, indicated by <strong>the</strong> blue contours, and it is visible<br />

from <strong>the</strong> lower image that this is associated with <strong>the</strong> production <strong>of</strong> Reynolds shear-stress<br />

(dashed lines § · ºñÀ indicate ). Though, it should be noted that <strong>the</strong> production <strong>of</strong> Reynolds<br />

shear stress induced by <strong>the</strong> sweeps is quite large as can be estimated from regions denoted<br />

by Q4 in <strong>the</strong> lower contour plot. Based on this experimental result it can be concluded that,<br />

in general, <strong>the</strong> lifting <strong>of</strong> low-speed streaks can be considered as a secondary motion which is<br />

induced by an interaction between a low-speed streak with a sweep, and <strong>the</strong> size and strength<br />

<strong>of</strong> <strong>the</strong> region, which moves away from <strong>the</strong> wall, is related to <strong>the</strong> momentum <strong>of</strong> <strong>the</strong> sweep. In<br />

addition it can be stated that <strong>the</strong> lifting <strong>of</strong> low-speed fluid into higher momentum <strong>flow</strong> regions<br />

128

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