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

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2.3 Registration <strong>of</strong> <strong>the</strong> particle images<br />

0.8<br />

0.8<br />

Intensity<br />

0.6<br />

0.4<br />

0.2<br />

0.6<br />

0.4<br />

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è 1é ê<br />

0<br />

−2 −1 0<br />

2<br />

è 1é ê<br />

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−2 −1 0<br />

2<br />

0.8<br />

0.8<br />

Intensity<br />

0.6<br />

0.4<br />

0.2<br />

0.6<br />

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x [pixel]<br />

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ê 1é è<br />

0<br />

−2 −1 0<br />

x [pixel]<br />

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ê 1é è<br />

FIGURE 2.10: Gaussian intensity distribution <strong>of</strong> a particle image (solid line) and its discrete representation<br />

as a function <strong>of</strong> <strong>the</strong> fill-factor, pixel response and sampling location (upper left to lower right).<br />

<strong>The</strong> dashed lines within <strong>the</strong> Gaussian distribution indicate <strong>the</strong> collected intensity calculated <strong>for</strong> <strong>the</strong> unbiased<br />

signal as a function <strong>of</strong> <strong>the</strong> linear pixel dimension and <strong>the</strong> long-dashed dotted line <strong>the</strong> modified<br />

intensity value (integration over <strong>the</strong> dotted graphs).<br />

Gaussian intensity distribution is not symmetric relative to <strong>the</strong> interface between two adjacent<br />

pixels, as shown in <strong>the</strong> two lower and <strong>the</strong> upper right graphs <strong>of</strong> figure 2.10, <strong>the</strong> unbiased signal<br />

increases continously from 0.48 to 0.68, in <strong>the</strong> example, until <strong>the</strong> centre <strong>of</strong> <strong>the</strong> pixel coincides<br />

with <strong>the</strong> maximum <strong>of</strong> <strong>the</strong> Gaussian curve (lower left graphs). Under <strong>the</strong>se conditions <strong>the</strong> greyvalues<br />

<strong>of</strong> <strong>the</strong> measured intensity is again completely symmetric with respect to <strong>the</strong> continuous<br />

distribution so that <strong>the</strong> exact location <strong>of</strong> <strong>the</strong> original function is identical with <strong>the</strong> discrete<br />

sample. To examine <strong>the</strong> behaviour <strong>of</strong> a small fill-ratio sensor, <strong>the</strong> intensity <strong>of</strong> <strong>the</strong> dashed and<br />

dashed dotted graphs can be compared at a particular sub-pixel location. A comparison indicates<br />

<strong>the</strong> minor importance <strong>of</strong> this parameter as long as <strong>the</strong> particle image size covers on<br />

average three pixels in each spatial direction. Under <strong>the</strong>se circumstances <strong>the</strong> measurement<br />

precision may be reduced as <strong>the</strong> differences between neighbouring pixel-intensities decrease<br />

while <strong>the</strong> influence <strong>of</strong> any superimposed noise increases, but this can be compensated by using<br />

<strong>the</strong> appropriate components <strong>for</strong> <strong>the</strong> experiment. If <strong>the</strong> particle image size is in <strong>the</strong> range <strong>of</strong><br />

27

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