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

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„ ƒ<br />

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

<strong>of</strong> <strong>the</strong> data. As <strong>the</strong> <strong>flow</strong> <strong>structures</strong> and <strong>the</strong>ir spatial organisation change while <strong>the</strong>y are transported<br />

downstream, <strong>the</strong> various correlation values yield in<strong>for</strong>mation about <strong>the</strong>ir life history.<br />

This is in some extent similar to <strong>the</strong> image analysis in PIV where <strong>the</strong> position, size, shape<br />

and intensity <strong>of</strong> <strong>the</strong> signal-peak in <strong>the</strong> correlation domain yield statistical in<strong>for</strong>mation about<br />

<strong>the</strong> size and shape <strong>of</strong> <strong>the</strong> particle images <strong>the</strong>mselves as well as in<strong>for</strong>mation about <strong>the</strong> magnitude,<br />

direction and homogeneity <strong>of</strong> <strong>the</strong> displacement <strong>of</strong> <strong>the</strong> particle ensemble in between <strong>the</strong><br />

two illuminations. <strong>The</strong> main difference lies in <strong>the</strong> fact that <strong>the</strong> fluid mechanical correlations<br />

presented in <strong>the</strong> following are ensemble averages calculated over hundreds <strong>of</strong> realizations,<br />

whereas in PIV <strong>the</strong> ensemble average is replaced by <strong>the</strong> spatial average <strong>of</strong> a single realization.<br />

This implies that in our case <strong>the</strong> statistical process leading to <strong>the</strong> fluid mechanical correlation<br />

functions must not necessarily be ergodic as required <strong>for</strong> PIV image analysis.<br />

Intensity<br />

Intensity<br />

x<br />

∆ ~ x<br />

∆τ<br />

∆t<br />

t<br />

x<br />

∆x<br />

∆τ<br />

…<br />

…<br />

…<br />

∆t<br />

∆ ~ x<br />

t<br />

FIGURE 7.2: Optimised light-sheet positioning to reduce loss-<strong>of</strong>-correlation due to unpaired particle<br />

image pairs, induced by out-<strong>of</strong>-plane (F† " ؇mù<br />

motion mm). Different light-sheet shadings indicate<br />

different states <strong>of</strong> polarisation. Left: Timing diagram <strong>for</strong> measuring all components <strong>of</strong> <strong>the</strong> space-time<br />

correlations tensor K+ Ø<br />

<strong>for</strong> and KJ various . Right: Timing diagram <strong>for</strong> measuring all components<br />

<strong>of</strong> <strong>the</strong> space-time correlations tensor <strong>for</strong> K‰ˆ<br />

Ø<br />

and various KJ .<br />

7.2 Statistical properties <strong>of</strong> <strong>the</strong> log-law region<br />

To ensure that <strong>the</strong> experimental arrangement was properly aligned relative to <strong>the</strong> <strong>flow</strong> direction,<br />

<strong>the</strong> main statistical <strong>flow</strong> properties were calculated and compared with <strong>the</strong> results<br />

presented in chapter 5. <strong>The</strong> top row <strong>of</strong> figure 7.3 shows <strong>the</strong> non-dimensional mean velocity<br />

pr<strong>of</strong>ile in linear and semi-logarithmic representation. It can be seen that <strong>the</strong> functional<br />

dependence agrees fairly well with <strong>the</strong> graph from <strong>the</strong> measurements presented in chapter 5.<br />

This demonstrates <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong> stereoscopic PIV method because <strong>the</strong> mean streamwise<br />

velocity in figure 7.3 corresponds to <strong>the</strong> out-<strong>of</strong>-plane velocity component in <strong>the</strong> present<br />

investigation. To estimate <strong>the</strong> quality <strong>of</strong> <strong>the</strong> camera and light-sheet alignment, <strong>the</strong> statistical<br />

properties <strong>of</strong> <strong>the</strong> fluctuations in <strong>the</strong> near-wall region were calculated. <strong>The</strong> distribution <strong>of</strong><br />

<strong>the</strong> velocity fluctuations and , <strong>the</strong> stream-wise vorticity a‹x and two components <strong>of</strong> <strong>the</strong><br />

|‹Š:Œ<br />

Reynolds stress tensor ( Πand | ) are exactly symmetrical so that a high <strong>flow</strong> quality and<br />

very accurate alignment <strong>of</strong> <strong>the</strong> laser and recording system can be assumed in <strong>the</strong> following.<br />

Any misalignment <strong>of</strong> <strong>the</strong> light-sheet with respect to <strong>the</strong> wall and mean <strong>flow</strong> direction or incorrect<br />

estimated camera positions would appear as a displacement <strong>of</strong> <strong>the</strong> distributions <strong>of</strong> certain<br />

magnitude and direction and, thus, indicate how to improve <strong>the</strong> setup or to correct <strong>the</strong> results.<br />

138

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