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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 />

300<br />

250<br />

200<br />

Vortex pair<br />

z<br />

+<br />

150<br />

Vortex pair<br />

Vortex pair<br />

100<br />

50<br />

0<br />

0 50 100 150 200 250 300 350 400 450 500 550<br />

300<br />

250<br />

??]<br />

x [???]<br />

z<br />

+<br />

200<br />

150<br />

Q2<br />

Q2<br />

Q4<br />

Q2<br />

100<br />

Q2<br />

50<br />

Q4<br />

0<br />

0 50 100 150 200 250 300 350 400 450 500 550<br />

x<br />

+<br />

y [???]<br />

x [???]<br />

FIGURE 6.27: Velocity fluctuations measured at Ó ® Ú¥Ø<br />

(top) and Reynolds stress component &C<br />

(bottom).<br />

tic velocity pattern, <strong>the</strong> velocity structure <strong>of</strong> <strong>the</strong> PIV measurements is analysed in stream-wise<br />

direction <strong>for</strong> various span-wise locations. For <strong>the</strong> comparison it is important to keep in mind<br />

that in <strong>the</strong> PIV experiment <strong>the</strong> spatial variation <strong>of</strong> <strong>the</strong> velocity is considered at a fixed time<br />

while <strong>the</strong> time signal <strong>of</strong> <strong>the</strong> velocity is considered at a fixed point in <strong>the</strong> hot wire investigation.<br />

<strong>The</strong> left image <strong>of</strong> figure 6.30 shows three typical instantaneous signals <strong>of</strong> <strong>the</strong> § -velocity<br />

component which nicely matches with <strong>the</strong> ensemble averaged pattern deduced from <strong>the</strong> hot<br />

wire measurements. <strong>The</strong> signals were extracted from figure 6.28 along <strong>the</strong> red lines located<br />

at Ï ® ¿ ÈÀ , 120 and 220. It can be clearly seen that <strong>the</strong> characteristic velocity pattern is<br />

130

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