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

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7.3 Spatio-temporal correlations with ×_ñò¬\<br />

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first order moments <strong>of</strong> <strong>the</strong> velocity fluctuations within this domain. It could be shown that<br />

<strong>the</strong> <strong>structures</strong> <strong>of</strong> <strong>the</strong> spatio-temporal auto-correlation functions <strong>of</strong> <strong>the</strong> stream-wise (ªS·· ) and<br />

span-wise (ªSÙ&Ù ) velocity fluctuations are quite similar (shape, size and temporal decay) when<br />

<strong>the</strong> span-wise and wall-normal dependence is considered, whereas <strong>the</strong>ir cross-correlation ªS·Ù<br />

is necessarily zero due to symmetry. Also, <strong>the</strong> characteristic shift <strong>of</strong> <strong>the</strong> largest correlation<br />

value towards higher velocity regions with time agrees well. <strong>The</strong> wall-normal correlations, on<br />

<strong>the</strong> o<strong>the</strong>r hand, are relatively small and <strong>the</strong>ir maximum decreases fast with increasing time. As<br />

a consequence, <strong>the</strong> spatial extent <strong>of</strong> regions where most <strong>of</strong> <strong>the</strong> Reynolds stresses are produced<br />

must be relatively limited. <strong>The</strong> correlation function <strong>of</strong> <strong>the</strong> stream-wise vorticity component<br />

also reveals a short spatio-temporal correlation length and a displacement towards higher velocity<br />

regions. Although a consistent interpretation <strong>of</strong> <strong>the</strong> presented results is conceivable, <strong>the</strong><br />

instantaneous velocity fields need to be analysed <strong>for</strong> fur<strong>the</strong>r evidence.<br />

y + ,∆t + )<br />

R uu<br />

(31+∆<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

20.4<br />

21.9<br />

27.3<br />

31.1<br />

34.6<br />

39.9<br />

43.3<br />

R uu<br />

(198+∆y + ,∆t + )<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

185.4<br />

198.4<br />

196.3<br />

198.5<br />

200.6<br />

205.2<br />

216.4<br />

y + ,∆t + )<br />

R uu<br />

(52+∆<br />

0.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

¨<br />

0<br />

50 ¨<br />

100<br />

¨<br />

© 150 200<br />

y + +∆y + <br />

© 250<br />

¨<br />

300<br />

34.1<br />

41.6<br />

48.5<br />

52.6<br />

56.6<br />

63.6<br />

77.1<br />

R uu<br />

(301+∆y + ,∆t + )<br />

0.6<br />

100<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

© 150<br />

¨<br />

200<br />

© 250 300<br />

y + +∆y + <br />

© 350<br />

¨<br />

400<br />

288.1<br />

298.6<br />

299.1<br />

301.3<br />

302.4<br />

305.6<br />

326.3<br />

y + ,∆t + )<br />

R uu<br />

(101+∆<br />

0.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

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0<br />

50 ¨<br />

100<br />

¨<br />

© 150 200<br />

y + +∆y +<br />

© 250<br />

¨<br />

300<br />

90.4<br />

99.4<br />

98.8<br />

101.2<br />

104.4<br />

111.2<br />

132.3<br />

R uu<br />

(398+∆y + ,∆t + )<br />

0.6<br />

200<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

© 250<br />

¨<br />

300<br />

© 350 400<br />

y + +∆y +<br />

© 450<br />

¨<br />

500<br />

394.7<br />

387.5<br />

398.6<br />

400.8<br />

402.9<br />

421.4<br />

0.2<br />

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0<br />

50 ¨<br />

100<br />

¨<br />

© 150 200<br />

y + +∆y +<br />

© 250<br />

¨<br />

300<br />

0.6<br />

300<br />

© 350<br />

¨<br />

400<br />

© 450 500<br />

y + +∆y +<br />

© 550<br />

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600<br />

FIGURE 7.14: Representation <strong>of</strong> <strong>the</strong> ˜ ·· correlation at ˜$ûšÀœ§§žž in <strong>the</strong> vicinity <strong>of</strong> <strong>the</strong> maximum<br />

<strong>for</strong> various wall distances © » <strong>of</strong> <strong>the</strong> fixed point and temporal separation between <strong>the</strong> measurements<br />

(ÉKøÓ» š Ð ž Æ ÏcÆ Ð§ÆØÆ ž Æ ÈÐ§Æ È7ÏcÆ ÈKÐ ž ).<br />

151

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