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

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tures keep <strong>the</strong>ir spatial organisation to a large extent while travelling down-stream by a few<br />

hundred wall units. <strong>The</strong> experimental results indicate that <strong>the</strong> maximum <strong>of</strong> <strong>the</strong> ªS·· correlation<br />

reach values above 0.8 <strong>for</strong> wall locations <strong>of</strong> <strong>the</strong> fixed point larger 100 wall units when <strong>the</strong><br />

<strong>flow</strong> moves 300 wall units in stream-wise direction, see page 152. For ¹ » %[Â <strong>the</strong> maximum<br />

reaches values above 0.6. This implies that <strong>the</strong> structural features <strong>of</strong> <strong>the</strong> velocity pattern conserve<br />

<strong>the</strong>ir identity to a large extent. This justifies <strong>the</strong> assumption made <strong>for</strong> <strong>the</strong> interpretation<br />

<strong>of</strong> <strong>the</strong> results in chapter 6. Fur<strong>the</strong>rmore, this result implies that <strong>the</strong> complex <strong>turbulent</strong> motion<br />

at a single point is a result <strong>of</strong> relatively simple <strong>coherent</strong> <strong>flow</strong> <strong>structures</strong> which are convecting<br />

downstream in <strong>for</strong>m <strong>of</strong> a frozen pattern. In this sense, <strong>the</strong> complexity is a result <strong>of</strong> <strong>the</strong> spatial<br />

distribution <strong>of</strong> <strong>the</strong> <strong>structures</strong> and <strong>the</strong>ir orientation relative to <strong>the</strong> main <strong>flow</strong> direction and not a<br />

result <strong>of</strong> a strong structural changes <strong>of</strong> <strong>the</strong> <strong>flow</strong> field itself. To examine <strong>the</strong> interaction <strong>of</strong> <strong>the</strong><br />

<strong>coherent</strong> <strong>flow</strong> structure below ¹&» ¬<br />

see page 144 and 145. <strong>The</strong>se functions imply that a vertical motion towards <strong>the</strong> wall induces<br />

a horizontal motion away from <strong>the</strong> centreline due to continuity, and a vertical motion at <strong>the</strong><br />

fixed point location ã with induces a horizontal motion ×pû ¬\ towards in <strong>the</strong> near-wall<br />

region and away from <strong>the</strong> centre at higher wall locations. This correlated motion indicates<br />

that a motion away from <strong>the</strong> wall is associated with <strong>the</strong> generation <strong>of</strong> a stream-wise vortex<br />

pair in accordance with <strong>the</strong> interpretation in chapter 6. To examine <strong>the</strong> characteristic features<br />

<strong>of</strong> <strong>the</strong> stream-wise vortices in detail and <strong>the</strong>ir <strong>significance</strong> <strong>for</strong> <strong>the</strong> <strong>turbulent</strong> <strong>mixing</strong>, instantaneous<br />

velocity fields were analysed, see page 156 to 160. It is shown that stream-wise vortices<br />

can be frequently observed in <strong>the</strong> near-wall region and also vortex pairs which transfer lowmomentum<br />

fluid away from <strong>the</strong> wall could be detected. However, <strong>the</strong> analysis shows that <strong>the</strong><br />

stream-wise length <strong>of</strong> <strong>the</strong>se vortices is not several thousand wall units in length, in agreement<br />

with <strong>the</strong> results in chapter 6, and <strong>the</strong> number <strong>of</strong> vortices which could be detected was relatively<br />

small relative to <strong>the</strong> number <strong>of</strong> low-speed streaks present in <strong>the</strong> near-wall region. This implies<br />

that <strong>the</strong> streaks are not generally flanked by stream-wise vortices as assumed in <strong>the</strong> literature.<br />

<strong>the</strong> cross-correlation ªSÔÙ and ªSÙ¥Ô was calculated,<br />

167

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