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

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

light-sheet by turning <strong>the</strong> cylindrical lens in <strong>the</strong> light-sheet optic. <strong>The</strong> observation angle <strong>for</strong><br />

each camera in angular imaging configuration with Scheimpflug correction is shown in <strong>the</strong><br />

following table along with <strong>the</strong> exact positions <strong>of</strong> <strong>the</strong> master cameras (1 and 2 in figure 7.1)<br />

with respect to <strong>the</strong> centre <strong>of</strong> <strong>the</strong> field <strong>of</strong> view (all asymmetries have been taken into account<br />

<strong>for</strong> <strong>the</strong> calculation <strong>of</strong> <strong>the</strong> three velocity components). Four 180 mm lenses (Carl Zeiss)<br />

camera Î [mm] Ï [mm] f@g [mm]<br />

¯<br />

[deg]<br />

1 -1570 1464 2143 42.9<br />

2 -1560 -1463 2140 43.2<br />

TABLE 7.1: Position and observation distance <strong>of</strong> <strong>the</strong> master cameras with respect to <strong>the</strong> centre <strong>of</strong> each<br />

field <strong>of</strong> view (meeting point <strong>of</strong> optical axis) and corresponding observation angles.<br />

a<br />

b<br />

40 mm separation<br />

~86°<br />

main <strong>flow</strong>-direction<br />

6<br />

5<br />

4<br />

7<br />

8<br />

test-section 3<br />

x<br />

2<br />

side window<br />

z<br />

1<br />

FIGURE 7.1: Schematic set-up <strong>of</strong> <strong>the</strong> recording system and light-sheet position <strong>for</strong> both experiments<br />

(different scales). 1-4 digital cameras, 5 lens, 6 mirror, 7 polarising beam-splitter cube, 8 absorbing<br />

material, a measurement location <strong>for</strong> 1st investigation (40 mm separation between both measurement<br />

planes in stream-wise direction), b measurement location <strong>for</strong> 2nd investigation (all measurement positions<br />

at <strong>the</strong> same location). Different light ray colours indicate different states <strong>of</strong> polarisation.<br />

were used <strong>for</strong> <strong>the</strong> measurements with an aperture <strong>of</strong> 8 and a magnification <strong>of</strong> 1/6 along <strong>the</strong><br />

principal axis <strong>of</strong> <strong>the</strong> lens. Due to <strong>the</strong> strong out-<strong>of</strong>-plane velocity component, as a result<br />

<strong>of</strong> <strong>the</strong> light-sheet orientation relative to <strong>the</strong> main <strong>flow</strong> direction, <strong>the</strong> light-sheet pairs with<br />

equal polarisation have been shifted in stream-wise direction as indicated in figure 7.2. This<br />

improves <strong>the</strong> signal to noise ratio, as <strong>the</strong> loss-<strong>of</strong>-correlation due to unpaired particle images is<br />

minimised without reducing <strong>the</strong> dynamic range and <strong>the</strong> spatial resolution. Decreasing Í_] or<br />

increasing <strong>the</strong> magnification <strong>of</strong> <strong>the</strong> imaging system would reduce <strong>the</strong> dynamic range or spatial<br />

resolution.<br />

136

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