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BSA Flow Software Installation and User's Guide - CSI

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Choice of polarization<br />

Choice of scattering angle<br />

3.) Connect the electrical cables from the <strong>BSA</strong> P processor signal processor<br />

channel U1 <strong>and</strong> U2 to the detector unit channels V1 <strong>and</strong> V2. Connect the<br />

electrical cables from the <strong>BSA</strong> P processor signal processor channel V1 <strong>and</strong><br />

V2 to the detector unit channels U1 <strong>and</strong> U2. This is necessary because the<br />

burst detector acts on channel U1 of the <strong>BSA</strong> P processor signal processor.<br />

The planar PDA attributes its name not only to the fact that the detectors lie<br />

in the same plane as the transmitting beams but also that the polarization lies<br />

in this plane (perpendicular polarization). Very early calculations indicated<br />

that visibility <strong>and</strong> the phase/diameter linearity was only acceptable for this<br />

polarization. Since the DualPDA receiving unit uses a common polarization<br />

filter for all channels, the polarization is chosen to be the same on all<br />

transmitted beams, i.e. parallel for the U-channels (green) <strong>and</strong> perpendicular<br />

for the V-channels (blue).<br />

This also corresponds to the preferred polarization in the case of the CPDA,<br />

i.e. the polarization at which a Brewster angle can be expected when<br />

working for instance with droplets in air (see 7.3 Setting up a PDA system).<br />

From section 7.3 Setting up a PDA system, we can expect scattering angles<br />

in the range 25° < Φ < 75° to be acceptable for the conventional PDA in the<br />

DualPDA. However further considerations must be given to the visibility<br />

<strong>and</strong> the phase/diameter linearity of the planar PDA as well as to the overall<br />

measurement size range. To investigate these influences, GLMT<br />

computations are recommended, some of which will be illustrated below.<br />

Prior to this however, some characteristic features of the DualPDA optical<br />

arrangement will be discussed. The following examples are valid for the<br />

st<strong>and</strong>ard DualPDA arrangement using either 160 mm or 400 mm lenses on<br />

the transmitting <strong>and</strong> receiving probes. To begin, the phase/diameter<br />

conversion factor for the CPDA <strong>and</strong> PPDA is computed using geometric<br />

optics, using the aperture centroid as the scattering direction. The results for<br />

the case of 160 mm focal length lenses is shown in Figure 7-52 an in Figure<br />

7-53 for various refractive indexes <strong>and</strong> for scattering angles in the range 20°<br />

to 70°. We can see that for scattering angle above 40-45deg, the V12 phase<br />

factor is low <strong>and</strong> phase factor ratio increases. This means that the<br />

measurement resolution will be very low for high scattering angles <strong>and</strong><br />

therefore it is not recommended to use such a configuration with DualPDA.<br />

Note This figure indicates that scattering angles beyond 40° would severely limit the PPDA at<br />

low relative refractive indexes. Values below 20° would lead to disturbances through<br />

diffraction. Therefore the operating range of 20° < Φ < 40° is expected to be most useful.<br />

<strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>:Reference guide 7-69

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