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

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3.2 Evaluation <strong>of</strong> stereo-scopic image pairs<br />

grid and Ï when a dot pattern is used) in order to determine <strong>the</strong> coordinates <strong>of</strong> <strong>the</strong> line crossing<br />

with sub-pixel accuracy 3 . After this step <strong>the</strong> imaging function between <strong>the</strong> image- and object<br />

plane can be changed from a discrete into a continuous representation by means <strong>of</strong> fitting a<br />

standard least squares surface to each <strong>of</strong> <strong>the</strong> image-object point sets, so that <strong>the</strong> first order<br />

projection matrix can be calculated <strong>for</strong> each observation direction along with <strong>the</strong> translation,<br />

rotation and magnification factor, [108].<br />

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(3.6)<br />

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In order to take into account aberrations <strong>of</strong> higher order and o<strong>the</strong>r non-linear distortions, <strong>the</strong><br />

second order projection in <strong>for</strong>m <strong>of</strong> equation (3.10) has to be applied. For this purpose <strong>the</strong><br />

coefficients <strong>of</strong> <strong>the</strong> first order projection matrix have to be used as an initial estimate to a<br />

Levenberg-Marquart non-linear least squares fitting algorithm.<br />

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(3.8)<br />

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r TK©<br />

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(3.9)<br />

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As both sets <strong>of</strong> trans<strong>for</strong>mation equations describe just a mapping between two planar domains<br />

without any three-dimensional in<strong>for</strong>mation, <strong>the</strong> location <strong>of</strong> <strong>the</strong> image with respect to <strong>the</strong> object<br />

has to be known in addition. This can be done ei<strong>the</strong>r directly, by measuring <strong>the</strong> exact camera<br />

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positions relative to <strong>the</strong> centre <strong>of</strong> <strong>the</strong> field <strong>of</strong> view, or indirectly by using <strong>the</strong> following set <strong>of</strong><br />

ù<br />

equations, see [56] <strong>for</strong> ma<strong>the</strong>matical details or [95] <strong>for</strong> <strong>the</strong> applicability in PIV.<br />

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ÒÓ (3.11)<br />

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<strong>The</strong> appearance <strong>of</strong> <strong>the</strong> -coordinate requires that <strong>the</strong> calibration procedure has to be repeated<br />

<strong>for</strong> different locations in order to determine all unknown coefficients. This is especially<br />

useful when <strong>the</strong> position <strong>of</strong> <strong>the</strong> cameras is not accessible or <strong>for</strong> applications in water, where<br />

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<strong>the</strong> air-glass-water interface has to be taken into E account.<br />

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3.2.2 Image warping<br />

Once <strong>the</strong> reconstruction coefficients have been properly determined, <strong>the</strong> trans<strong>for</strong>mation equations<br />

can be applied to de<strong>for</strong>m each acquired, single-exposed image in such a way that <strong>the</strong><br />

magnification factor is constant across <strong>the</strong> back-projected image and <strong>the</strong> field <strong>of</strong> view is identical<br />

<strong>for</strong> all acquired images. Using this technique optical parameters such as <strong>the</strong> focal length<br />

3 As this method is quite time consuming, Hough trans<strong>for</strong>mation methods are usually applied in this <strong>the</strong>sis to<br />

find <strong>the</strong> coordinates <strong>of</strong> <strong>the</strong> line crossings, see [18].<br />

43

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