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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 />

function is not necessarily an even function with a Í5Î ¿ À maximum at in contrast to <strong>the</strong><br />

primary correlations, but <strong>the</strong>re exists still an important symmetry property when <strong>the</strong> random<br />

variables and are interchanged, namely Ã Ñ Ë ¹ Í5Î|¼ ¿ ÃË Ñ ¹ Í5Î|¼ . <strong>The</strong> left column<br />

§<br />

in figure 6.8 shows · Ñ <strong>the</strong> correlation function with <strong>the</strong> component fixed and § shifted in<br />

ÃË<br />

<strong>the</strong> two homogeneous directions. First <strong>of</strong> all it should be noted that <strong>the</strong> sign · Ñ <strong>of</strong> ÃË again<br />

indicates that <strong>the</strong> transport <strong>of</strong> relatively low-momentum fluid outward into higher speed re-<br />

) and <strong>the</strong> movement <strong>of</strong> high-momentum fluid toward <strong>the</strong> wall into<br />

½þÀ<br />

(§ßºöÀ gions and<br />

lower speed regions ·<br />

and · º¤À ) are <strong>the</strong> predominant processes in <strong>the</strong> near-wall region.<br />

(§N½¤À<br />

In addition, <strong>the</strong> strong elliptical shape implies that <strong>the</strong> <strong>turbulent</strong> <strong>mixing</strong> in <strong>the</strong> wall-normal<br />

direction is related to <strong>the</strong> low-speed <strong>structures</strong> represented à êJî Ñí êJî Ñí by in figure 6.7. But obviously<br />

only a small part <strong>of</strong> <strong>the</strong> low-momentum <strong>structures</strong> shows a correlated motion in both<br />

−0.6<br />

−0.6<br />

R vu<br />

−0.4<br />

−0.2<br />

æ<br />

∆x + =+ 5<br />

∆x + =−12<br />

∆x + =−17<br />

R vu<br />

−0.4<br />

−0.2<br />

æ<br />

∆z + =42<br />

∆z + =50<br />

∆z + =68<br />

0.0<br />

0.0<br />

R uw<br />

ã 0.2<br />

−300 −200 −100 0 100<br />

∆x +<br />

−0.6<br />

−0.4<br />

−0.2<br />

0.0<br />

200<br />

ã<br />

æ<br />

∆x + =−49<br />

∆x + =−57<br />

∆x + =−57<br />

300<br />

ã<br />

R uw<br />

â 0.2<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

−0.4<br />

−0.2<br />

0.0<br />

0.2<br />

æ<br />

∆z + =27<br />

∆z + =38<br />

∆z + =50<br />

150 â<br />

R vw<br />

ã 0.2<br />

−300 −200 −100 0 100<br />

∆x +<br />

−0.6<br />

−0.4<br />

−0.2<br />

200<br />

ã<br />

æ<br />

∆x + =−10<br />

∆x + =−28<br />

∆x + =−35<br />

300<br />

ã<br />

R vw<br />

â 0.4<br />

−150 −100 −50 0 50 100<br />

∆z +<br />

−0.4<br />

−0.2<br />

0.0<br />

æ<br />

∆z + =−16<br />

∆z + =−24<br />

∆z + =−31<br />

150 â<br />

0.0<br />

0.2<br />

ã<br />

0.2<br />

−300 −200 −100 0 100<br />

∆x<br />

200<br />

ã<br />

300<br />

ã<br />

â 0.4<br />

−150 −100 −50 0 50 100<br />

∆z<br />

150 â<br />

FIGURE 6.9: One-dimensional spatial cross-correlation function <strong>of</strong> Reynolds stress components measured<br />

at different wall-normal location (Solid graph: Ó ® Ô Ü Ø<br />

. Dotted graph: Ó ® Ô×Ú¥Ø<br />

. Dashed graph:<br />

Ó ®NÔõÖ¥Ø<br />

) as a function <strong>of</strong> ®<br />

and ®<br />

. <strong>The</strong> symbols indicate <strong>the</strong> maximum <strong>of</strong> correlation and <strong>the</strong><br />

legend <strong>the</strong> distance from <strong>the</strong> minimum to <strong>the</strong> origin.<br />

110

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