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BSA Flow Software Installation and User's Guide - CSI

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This is the principle of the spherical check illustrated for the conventional<br />

PDA in Figure 7-24: the phase differences Φ 12 <strong>and</strong> Φ 13 should point at the<br />

same diameter, D. For the DualPDA the corresponding phase differences<br />

would be Φ U12 <strong>and</strong> Φ V12 (see 7.2.2 The concept of the DualPDA)<br />

If the two local curvatures differ, Φ 12 <strong>and</strong> Φ 13 will point at diameter values<br />

differing by ∆D (Figure 7-24).<br />

Figure 7-24. Difference, ∆D, in the diameter value corresponding to the two phase<br />

differences Φ12 <strong>and</strong> Φ13.<br />

One validation criterion in <strong>BSA</strong> flow software is the maximum allowable<br />

deviation from sphericity. Thus, if ∆D exceeds a certain limit set by the<br />

user, the particle is not accepted.<br />

Phase measurements will always have some associated uncertainty (Figure<br />

7-25). The detectors will be specified within certain tolerances, partly there<br />

will be noise present influencing the accuracy.<br />

Figure 7-25: Effect of uncertainty in the estimation of the phase difference.<br />

Concentration Apart from size <strong>and</strong> velocity, the PDA can also be used for measuring<br />

measurements particle concentration. A description of how this is achieved is given in<br />

chapter 7.11 (Mean diameters <strong>and</strong> algorithms for concentration <strong>and</strong> flux<br />

measurements).<br />

<strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>:Reference guide 7-29

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