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Coherent Backscattering from Multiple Scattering Systems - KOPS ...

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5 Experiments<br />

1<br />

0.8<br />

data − ( n water<br />

= 1.334 , n particle<br />

= 1.519 ) .<br />

data − ( n water<br />

= 1.334 , n particle<br />

= 1.521 )<br />

data − ( n water<br />

= 1.334 , n particle<br />

= 1.523 )<br />

intensity [a.u.]<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 0.05 0.1 0.15 0.2<br />

scattering angle θ ms<br />

[deg]<br />

Figure 5.18: <strong>Coherent</strong> backscattering cone of a fluidized bed. To obtain the coherent<br />

backscattering cone, three Mie distributions (stretched along the angular axis to match<br />

the slope of the first maximum of the data) with different zero levels were subtracted<br />

<strong>from</strong> the measured intensity distribution depicted in fig. 5.17. The angular width of the<br />

cone can be read <strong>from</strong> the graph to an accuracy of about 15%.<br />

The graph also shows that the actual distribution of particle sizes in the sample differs slightly<br />

<strong>from</strong> the one measured beforehand – either because the size distribution in the fluidized bed is<br />

not homogenous or because the size distribution changed during the experiments – as the first<br />

maxima of measured data and Mie theory do not fit. For the evaluation the Mie distribution<br />

was therefore stretched to match the measured intensity distribution. This is acceptable as the<br />

intensity characteristics are always the same at small angles; however, the zero level of the Mie<br />

distribution varies with the input parameters, so that the width of the backscattering cone is<br />

known only to an accuracy of about 15% (fig. 5.18).<br />

The transport mean free path of a fluidized bed<br />

The first backscattering experiments were performed on a fluidized bed of water and soda<br />

lime glass spheres with particle diameters around 150 µm. The transport mean free path was<br />

expected to be proportional to the distance between the particles in the fluidized bed. So the<br />

backscattering was measured for different flux rates in the bed, resulting in particle volume<br />

fractions between 39% and 58% (fig. 5.19). However, due to strong fluctuations in the data no<br />

real trend in the width of the backscattering cone can be observed – which does not necessarily<br />

mean that there is none. Here additional speckles <strong>from</strong> static particles stuck at the container<br />

surface do have a rather disadvantageous impact.<br />

66

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