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

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varying signal can be trans<strong>for</strong>med into a time dependent signal at a fixed point, whe<strong>the</strong>r a characteristic<br />

velocity pattern, that was observed in <strong>the</strong> past by using hot-wire probes, is related to<br />

<strong>the</strong> motion <strong>of</strong> particular <strong>coherent</strong> <strong>structures</strong>. <strong>The</strong> results <strong>of</strong> this chapter are partially published<br />

in [41].<br />

Chapter 7 focuses finally on <strong>the</strong> wall-normal span-wise plane ([-plane) investigation <strong>of</strong><br />

<strong>the</strong> <strong>turbulent</strong> boundary layer by means <strong>of</strong> multiplane stereo PIV and*1¥¥¥.<br />

<strong>The</strong>se investigations were mainly per<strong>for</strong>med to examine <strong>the</strong> validity <strong>of</strong> <strong>the</strong> frozen pattern<br />

concept, applied in chapter 6, and to prove <strong>the</strong> existence <strong>of</strong> stream-wise vortices in <strong>the</strong> nearwall<br />

region and <strong>the</strong>ir <strong>significance</strong> <strong>for</strong> <strong>the</strong> <strong>turbulent</strong> <strong>mixing</strong> normal to <strong>the</strong> wall. Two independent<br />

experiments are described with different spatial separation between <strong>the</strong> measurement planes<br />

in stream-wise direction (<br />

at&%<br />

£g¥) and<br />

£<br />

and various temporal delays between a pair<br />

54¥.¥<br />

<strong>of</strong> measurements. Due to <strong>the</strong> widespread opinion that reliable experimental results are very<br />

difficult to achieve when <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> light-sheet is perpendicular to <strong>the</strong> main <strong>flow</strong><br />

direction, in section 7.2 <strong>the</strong> statistical results are validated against <strong>the</strong> results presented in <strong>the</strong><br />

chapter 5. In section 7.2.2 <strong>the</strong> structural features <strong>of</strong> <strong>the</strong> <strong>coherent</strong> <strong>flow</strong> <strong>structures</strong> are displayed<br />

and <strong>the</strong> model assumption made <strong>for</strong> <strong>the</strong> interpretations <strong>of</strong> <strong>the</strong> results presented in chapter<br />

¢¡f£g¥ h¡©<br />

5<br />

and 6 will be examined. In section 7.4 <strong>the</strong> decay <strong>of</strong> <strong>the</strong> <strong>coherent</strong> <strong>structures</strong> with increasing<br />

time is investigated as a function <strong>of</strong> <strong>the</strong> wall distance to validate <strong>the</strong> frozen pattern hypo<strong>the</strong>sis.<br />

In section 7.5 <strong>the</strong> existence and relevance <strong>of</strong> <strong>the</strong> stream-wise vortex pairs <strong>for</strong> <strong>the</strong> <strong>turbulent</strong><br />

<strong>mixing</strong> in wall bounded <strong>flow</strong>s is finally examined and <strong>the</strong> concept <strong>of</strong> hairpin or horseshoes<br />

like <strong>structures</strong> is discussed as well as <strong>the</strong>ir connection with shear-layers and streaks. Parts <strong>of</strong><br />

this chapter are already published in [49]. As <strong>the</strong> fully-developed <strong>turbulent</strong> boundary layer<br />

<strong>flow</strong> along a flat plate is considered as one <strong>of</strong> <strong>the</strong> basic academic <strong>flow</strong>s which is accessible by<br />

Direct Numerical Simulations (DNS), and a test case <strong>for</strong> <strong>the</strong> validation <strong>of</strong> turbulence models<br />

required <strong>for</strong> Large Eddy (LES) and Reynolds Averaged Navier-Stokes Simulations (RANS),<br />

<strong>the</strong> statistical results presented in chapter 5 to 7 are displayed in various representations to<br />

simplify a comparison in <strong>the</strong> future.<br />

11

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