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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 />

velocity fluctuations measured at «¢ÀÁ À and ª¡À (top to bottom). Clearly noticeable is<br />

<strong>the</strong> characteristic elliptical shape <strong>of</strong> both correlations, with <strong>the</strong> principal axis in stream-wise<br />

direction, as well as <strong>the</strong> strong dependence <strong>of</strong> <strong>the</strong> correlation width from <strong>the</strong> wall distances<br />

­.®zÊ<br />

in accordance with [44] and <strong>the</strong> results presented in section 5.3.2. However, <strong>the</strong> most striking<br />

feature, which could not be established be<strong>for</strong>e, is <strong>the</strong> variation <strong>of</strong> <strong>the</strong> size and span-wise<br />

location <strong>of</strong> <strong>the</strong> weak negative correlation regions ÃËÌË <strong>of</strong> , when approaching <strong>the</strong> wall. This<br />

is clearly visible in <strong>the</strong> upper right plot <strong>of</strong> figure 6.7 where <strong>the</strong> span-wise dependence <strong>of</strong> this<br />

correlation Í5Î ® ¿ À at is shown in wall-units. <strong>The</strong> location <strong>of</strong> <strong>the</strong> minima is highlighted<br />

with symbols and <strong>the</strong> legend reveals <strong>the</strong> corresponding displacement <strong>of</strong> <strong>the</strong> symbols from <strong>the</strong><br />

maximum <strong>of</strong> correlation, located ÍeÏ ® ¿ À at . <strong>The</strong> range <strong>of</strong> correlation values indicates a large<br />

range <strong>of</strong> scales and <strong>the</strong> minima imply a span-wise periodicity whose wavelength strongly increases<br />

with increasing wall distance. From <strong>the</strong> negative correlation regions, <strong>the</strong> existence <strong>of</strong><br />

stream-wise vortices can be concluded. However, it should be noted that <strong>the</strong>ir length is not<br />

+ +<br />

R uu (y =30)<br />

R (y =30)<br />

vv<br />

∆ z +<br />

∆ z +<br />

∆ z<br />

+<br />

+<br />

R uu (y =20)<br />

+<br />

R uu (y =10)<br />

+<br />

R vv (y =20)<br />

+<br />

R vv (y =10)<br />

∆x + ∆x +<br />

FIGURE 6.6: Two-dimensional spatial correlation function <strong>of</strong> fluctuating stream-wise ÐÒÑ˜Ñ velocity<br />

(left) and wall-normal Ð ËÌË velocity (right) measured Ó ®ÕÔ×֥آÙÛÚ¥Ø<br />

at Ü Ø<br />

and (top to bottom).<br />

106

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