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

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æ<br />

ã<br />

ã<br />

ã<br />

H<br />

H<br />

H<br />

I<br />

I<br />

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ã<br />

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

Figure 6.15 and figure 6.16 present <strong>the</strong> cross-correlations where <strong>the</strong> span-wise velocity component<br />

is involved. <strong>The</strong> similar shape <strong>of</strong> <strong>the</strong> correlations is clearly visible, but <strong>the</strong> larger extent<br />

<strong>of</strong> <strong>the</strong> Ã Ñ function with respect to ÃË should be noted and <strong>the</strong> difference in <strong>the</strong> maximum <strong>of</strong><br />

correlation which indicates that <strong>the</strong> ÃË correlation exceeds <strong>the</strong> coherence <strong>of</strong> <strong>the</strong> Ã Ñ$ function.<br />

This is fully in accordance with <strong>the</strong> analysis in <strong>the</strong> previous section. Of fundamental importance<br />

are <strong>the</strong> differences in <strong>the</strong> fine structure if <strong>the</strong> correlation is considered as a function <strong>of</strong><br />

<strong>the</strong> temporal delay and <strong>the</strong> structure dependent convection velocity highlighted quantitatively<br />

in figure 6.17 to figure 6.19. Only a line <strong>of</strong> <strong>the</strong> data extracted from <strong>the</strong> two-dimensional correlation<br />

functions along <strong>the</strong> Î -coordinate through <strong>the</strong> maximum <strong>of</strong> correlation is shown here.<br />

1.0<br />

1.0<br />

R uu<br />

(∆t + )<br />

0.8<br />

0.6<br />

0.4<br />

æ<br />

∆x + =18<br />

∆x + =64<br />

∆x + =118<br />

t + )<br />

R uu<br />

(∆<br />

0.8<br />

0.6<br />

0.4<br />

I<br />

∆x + =−27<br />

∆x + =28<br />

∆x + =87<br />

0.2<br />

0.2<br />

ã<br />

0.0<br />

−300 −200 −100 0 100<br />

∆x<br />

1.0<br />

200<br />

ã<br />

300<br />

ã<br />

0.0<br />

−300 −200 −100<br />

1.0<br />

ã<br />

0<br />

∆x<br />

+<br />

100<br />

ã<br />

200<br />

ã<br />

300<br />

ã<br />

R (−u)(−u)<br />

(∆t + )<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

æ<br />

∆x + =14<br />

∆x + =49<br />

∆x + =93<br />

t + )<br />

R (−u)(−u)<br />

(∆<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

∆x + =−17<br />

∆x + =29<br />

∆x + =78<br />

ã 0.0<br />

−300 −200 −100 0 100<br />

∆x +<br />

1.0<br />

200<br />

ã<br />

300<br />

ã<br />

0.0<br />

−300 −200 −100<br />

1.0<br />

ã<br />

0<br />

∆x +<br />

100<br />

ã<br />

200<br />

ã<br />

300<br />

ã<br />

R (+u)(+u)<br />

(∆t + )<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

æ<br />

∆x + =37<br />

∆x + =86<br />

∆x + =159<br />

t + )<br />

R (+u)(+u)<br />

(∆<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

I<br />

∆x + =−48<br />

∆x + =20<br />

∆x + =98<br />

ã<br />

0.0<br />

−300 −200 −100 0 100<br />

∆x<br />

200<br />

ã<br />

300<br />

ã<br />

0.0<br />

−300 −200 −100<br />

ã<br />

0<br />

∆x<br />

+<br />

100<br />

ã<br />

200<br />

ã<br />

300<br />

ã<br />

FIGURE 6.17: One-dimensional spatio-temporal correlation function <strong>of</strong> stream-wise velocity fluctuation<br />

(top), <strong>the</strong> low-momentum fluctuations in stream-wise Ð î Ñ î Ñ direction (centre) and <strong>the</strong><br />

ÐÒјÑ<br />

high-momentum stream-wise Ð ® Ñ ® Ñ fluctuations (bottom) measured Ó ® Ü Ø<br />

at (left column) and<br />

® Ú¥Ø<br />

(right column) and different time delays between a pair <strong>of</strong> measurements (KJ ® ú ù<br />

solid<br />

Ó<br />

J ® Ø<br />

line, dotted KJ ® L6 ù<br />

line, dashed line). <strong>The</strong> symbol indicates <strong>the</strong> maximum <strong>of</strong> correlation<br />

and <strong>the</strong> legend shows <strong>the</strong> exact position in wall-units.<br />

118

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