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

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7 Investigation <strong>of</strong> <strong>the</strong> yz-plane<br />

by using <strong>the</strong> results from chapter 5. ×_ì˻߬<br />

¿ °<br />

For (lower left row <strong>of</strong> figure 7.15) <strong>the</strong> travelling<br />

distance is around 240 wall-units (75% <strong>of</strong> <strong>the</strong> separation between measurement planes)<br />

<strong>for</strong> <strong>the</strong> near-wall <strong>structures</strong>, but <strong>the</strong> <strong>structures</strong> ¹&» w at already reach <strong>the</strong> second observation<br />

plane as <strong>the</strong> mean convection velocity varies between 18 ¹ » ¬'w <strong>for</strong> and ¯cä »<br />

<strong>for</strong> ¿#")( . This can be directly estimated from <strong>the</strong> height <strong>of</strong> <strong>the</strong> correlation maximum<br />

¹&»À¬+*<br />

in <strong>the</strong> upper right graph <strong>of</strong> figure 7.15. While <strong>the</strong> correlation maximum already decreases<br />

<strong>for</strong> fixed point locations ¹¥» c at a gradual increase can be observed <strong>for</strong> <strong>the</strong> near-wall<br />

correlations. All correlation maxima increase with ×_ì increasing while <strong>the</strong> maximum correlation<br />

always remains lower near <strong>the</strong> wall. As <strong>the</strong> difference in height is quite large, structural<br />

changes or variation in <strong>the</strong> organisation <strong>of</strong> <strong>the</strong> <strong>structures</strong> closer to <strong>the</strong> wall (strong variation<br />

<strong>of</strong> <strong>the</strong> structure location from one time-step to <strong>the</strong> next) need to be assumed <strong>for</strong> this effect.<br />

This assumption is strongly supported by <strong>the</strong> fact that both, integral and dissipative, length<br />

scales significantly increase in <strong>the</strong> two last rows. Translated in <strong>the</strong> language <strong>of</strong> PIV image<br />

analysis, this effect corresponds to loss <strong>of</strong> pairs (resulting in a lower correlation coefficient)<br />

1<br />

1<br />

0.8<br />

0.8<br />

R ww<br />

(∆t + =0)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

R ww<br />

(∆t + =20)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

1<br />

,<br />

0<br />

100<br />

,<br />

,<br />

200 300<br />

y + +∆y + -<br />

400<br />

,<br />

500<br />

,<br />

−0.2<br />

1<br />

,<br />

0<br />

100<br />

,<br />

,<br />

200 300<br />

y + +∆y + -<br />

400<br />

,<br />

500<br />

,<br />

0.8<br />

0.8<br />

R ww<br />

(∆t + =8)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

R ww<br />

(∆t + =25)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

1<br />

,<br />

0<br />

100<br />

,<br />

200<br />

,<br />

y + +∆y +<br />

300<br />

,<br />

400<br />

,<br />

500<br />

,<br />

−0.2<br />

1<br />

,<br />

0<br />

100<br />

,<br />

200<br />

,<br />

y + +∆y +<br />

300<br />

,<br />

400<br />

,<br />

500<br />

,<br />

0.8<br />

0.8<br />

R ww<br />

(∆t + =15)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

R ww<br />

(∆t + =30)<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

,<br />

0<br />

100<br />

,<br />

,<br />

200 300<br />

y + +∆y + -<br />

400<br />

,<br />

500<br />

,<br />

−0.2<br />

,<br />

0<br />

100<br />

,<br />

,<br />

200 300<br />

y + +∆y + -<br />

400<br />

,<br />

500<br />

,<br />

FIGURE 7.17: ˜ Ù¥Ù correlation measured at ˜#š œ§§žž and © » š Ñ ž Æ Î§ž ÆËÏ ž ÆÐ žž ÆËÑ ž±ž Æ Î§žž ÆÓÒ žž (see<br />

location <strong>of</strong> <strong>the</strong> maximum) <strong>for</strong> various temporal delays (see axis label).<br />

154

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