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

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6.2 Statistical properties <strong>of</strong> <strong>the</strong> buffer layer<br />

as long as expected by o<strong>the</strong>r authors as can be seen from <strong>the</strong> stream-wise extension <strong>of</strong> <strong>the</strong><br />

negative correlation region in figure 6.6. In case <strong>of</strong> <strong>the</strong> Ã Ñ‘Ñ correlation, shown in <strong>the</strong> upper<br />

left plot <strong>of</strong> figure 6.7, only <strong>the</strong> function measured at ­®ÝÊ<br />

direction and reveals a weak minimum at Í5Î ® ÊßÞ « , while <strong>the</strong> o<strong>the</strong>rs slowly converge to zero<br />

with increasing ÍeÏ ®<br />

. This indicates a decreasing dynamic velocity range with increasing wall<br />

distance, as expected from <strong>the</strong> à §(á pr<strong>of</strong>iles in figure 5.3, and implies that <strong>the</strong> <strong>coherent</strong> velocity<br />

regions rapidly loose <strong>the</strong>ir identity with increasing wall distance ­ . To deduce <strong>the</strong> statistical<br />

properties <strong>of</strong> <strong>the</strong> dominant low- and high-momentum <strong>flow</strong> <strong>structures</strong> which are convecting<br />

downstream, <strong>the</strong> measured data was subdivided according to <strong>the</strong> sign <strong>of</strong> <strong>the</strong> stream-wise velocity<br />

fluctuation be<strong>for</strong>e calculating <strong>the</strong> correlation functions. This conditional correlation<br />

approach allows to identify <strong>the</strong> <strong>structures</strong> associated with ejection and sweeps <strong>for</strong> instance.<br />

ª¡À changes its sign in span-wise<br />

R uu<br />

R uu<br />

(u0)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

æ<br />

∆z + =63<br />

æ<br />

∆z + =46/112<br />

∆z + =46<br />

∆z + =70<br />

æ<br />

∆z + =70<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z<br />

150 â<br />

150 â<br />

150 â<br />

R vv<br />

R vv<br />

(u0)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

æ<br />

∆z + =31<br />

∆z + =44<br />

∆z + =53<br />

æ<br />

∆z + =35<br />

∆z + =38<br />

∆z + =42<br />

æ<br />

∆z + =27<br />

∆z + =44<br />

∆z + =53<br />

â −0.2<br />

−150 −100 −50 0 50 100<br />

∆z<br />

150 â<br />

150 â<br />

150 â<br />

FIGURE 6.7: One-dimensional spatial correlation function <strong>of</strong> fluctuating stream-wise and wall-normal<br />

velocity components measured at Ó ® Ô<br />

graph) as a function <strong>of</strong> <strong>the</strong> span-wise coordinate. <strong>The</strong> symbols indicate <strong>the</strong> location <strong>of</strong> <strong>the</strong> minimum<br />

and <strong>the</strong> legend <strong>the</strong> displacement <strong>of</strong> <strong>the</strong> minimum from <strong>the</strong> origin.<br />

Ü Ø<br />

(solid graph), Ó ® Ô×Ú¥Ø<br />

(dotted graph) and Ó ® ÔéÖ¥Ø<br />

(dashed<br />

107

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