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Application and Optimisation of the Spatial Phase Shifting ...

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104 Quantification <strong>of</strong> displacement-measurement errors<br />

grey value<br />

224<br />

192<br />

160<br />

128<br />

96<br />

64<br />

32<br />

0<br />

raw data<br />

9x9 median<br />

320 370 420 470 520 570<br />

x -position/pixel<br />

Fig. 4.3: Deterministically distorted fringe pr<strong>of</strong>ile due to wrong phase shift; filtering in 2D by <strong>the</strong> sine-cosine<br />

method with 9<br />

9-median windows.<br />

From this, it gets clear that filtering sawtooth images to obtain reference data is always only an<br />

approximation. This should perform well enough in most cases but seems inappropriate for us since <strong>the</strong>re<br />

are some extreme fringe densities <strong>and</strong> noise levels to be explored. And finally, <strong>the</strong> filter size cannot be<br />

st<strong>and</strong>ardised, <strong>the</strong> best choice would change from image to image <strong>and</strong> still remain a matter <strong>of</strong> judgement.<br />

4.1.2.3 Composite method<br />

Recently it has been demonstrated that a very good filter can be implemented by using <strong>the</strong> sine-cosine<br />

method with a small filter size toge<strong>the</strong>r with a large number <strong>of</strong> iterations [Aebi99]; <strong>the</strong> peculiarity <strong>of</strong> this<br />

algorithm is that <strong>the</strong> phase is always re-calculated between <strong>the</strong> iterations. Once again, <strong>the</strong> phasor<br />

interpretation assists in underst<strong>and</strong>ing this qualitatively: by determining <strong>the</strong> phases <strong>and</strong> re-deriving sine<br />

<strong>and</strong> cosine from <strong>the</strong>m, <strong>the</strong> length <strong>of</strong> <strong>the</strong> phasors is re-set to unity in each iteration, which counteracts <strong>the</strong><br />

contrast attenuation mentioned above <strong>and</strong> preserves any phase detail in <strong>the</strong> image that survives a single<br />

run <strong>of</strong> <strong>the</strong> filter kernel. Hence, one can in principle use arbitrarily many iterations <strong>and</strong> <strong>the</strong>refore eliminate<br />

<strong>the</strong> speckle noise almost completely. This seems to be a promising method to generate near-ideal<br />

reference data from whatever input fringe pattern. But still <strong>the</strong> restriction is that <strong>the</strong> filter size must be<br />

optimised by <strong>the</strong> operator; <strong>and</strong> also, depending on <strong>the</strong> accuracy required, <strong>the</strong> number <strong>of</strong> iterations may<br />

become very large. It was also observed that at <strong>the</strong> borders <strong>of</strong> <strong>the</strong> image <strong>and</strong>/or at phase discontinuities in<br />

<strong>the</strong> image, <strong>the</strong> phase pr<strong>of</strong>ile gets more <strong>and</strong> more distorted with increasing number <strong>of</strong> iterations.<br />

4.1.2.4 Comparing unwrapped data<br />

The problem <strong>of</strong> white-black edges in <strong>the</strong> image can also be circumvented by unwrapping <strong>the</strong> phase before<br />

comparing raw <strong>and</strong> smoo<strong>the</strong>d data. Clearly, <strong>the</strong> raw image must not be filtered before unwrapping, which<br />

restricts <strong>the</strong> application <strong>of</strong> this method to ra<strong>the</strong>r good results with low to medium noise <strong>and</strong> moderate<br />

fringe density. Even <strong>the</strong>n, <strong>the</strong> result will not be a direct conversion <strong>of</strong> phase to displacement, since almost

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