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

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6.3 Spatio-temporal buffer layer statistics<br />

First <strong>of</strong> all it can be seen that <strong>the</strong> shift <strong>of</strong> <strong>the</strong> maximum (indicated by <strong>the</strong> symbols and <strong>the</strong><br />

legend) strongly depends on <strong>the</strong> sign <strong>of</strong> <strong>the</strong> stream-wise velocity fluctuation considered <strong>for</strong><br />

<strong>the</strong> calculation <strong>of</strong> <strong>the</strong> conditional correlation and from <strong>the</strong> wall-distance <strong>for</strong> all correlations.<br />

This becomes clear as <strong>structures</strong> whose velocity is larger than <strong>the</strong> mean velocity are travelling<br />

faster. Secondly, it turns out that <strong>the</strong> height <strong>of</strong> <strong>the</strong> conditional correlations is always lower<br />

than <strong>the</strong> correlations based on all fluctuations. Finally, it should be noted by comparing <strong>the</strong><br />

values in <strong>the</strong> legend that <strong>the</strong> movement <strong>of</strong> high-speed <strong>structures</strong> towards and away from <strong>the</strong><br />

wall differs to a large extent. Since <strong>the</strong> distance between each <strong>of</strong> a pair <strong>of</strong> measurement planes<br />

was 10 wall-units, it is possible to obtain in<strong>for</strong>mation about <strong>the</strong> extension <strong>of</strong> <strong>the</strong> <strong>structures</strong><br />

1.0<br />

1.0<br />

R vv<br />

(∆t + )<br />

0.8<br />

0.6<br />

0.4<br />

æ<br />

∆x + =−41<br />

∆x + =13<br />

∆x + =67<br />

t + )<br />

R vv<br />

(∆<br />

0.8<br />

0.6<br />

0.4<br />

I<br />

∆x + =−52<br />

∆x + =10<br />

∆x + =73<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 vv<br />

(∆t + ,u0)<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

∆x + =−56<br />

∆x + =12<br />

∆x + =80<br />

ã 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 />

100<br />

ã<br />

200<br />

ã<br />

300<br />

ã<br />

FIGURE 6.18: One-dimensional spatio-temporal correlation function <strong>of</strong> wall-normal velocity fluctuation<br />

Ð ËÛË (top), and correlations <strong>of</strong> wall-normal fluctuation extracted in regions with N Ø<br />

(centre) and<br />

O! Ø<br />

(bottom) measured at Ó ® Ü Ø<br />

(left column) and Ó ® Ú¥Ø<br />

(right column) and different time delays<br />

between a pair <strong>of</strong> measurements (KJ ® ú ù<br />

solid line, KJ ® Ø<br />

dotted line, J ® P6 ù<br />

dashed<br />

line). <strong>The</strong> symbol indicates <strong>the</strong> maximum <strong>of</strong> correlation and <strong>the</strong> legend shows <strong>the</strong> exact position in<br />

wall-units.<br />

119

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