Optical Particle Sizing 1988
DOI: 10.1007/978-1-4757-1983-3_36
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Size and Velocity Measurements of Spherical Particles in Multiphase Flows and the Prediction of Absolute Particle Concentrations

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Cited by 6 publications
(3 citation statements)
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“…The principles of phase-Doppler anemometry for determining simultaneously velocity and size distributions of suspended spherical particles were first presented by Durst and Zaré [1]. Subsequent contributions to the development of phase-Doppler anemometry, for example [2][3][4] were essential to the development of the technique and the recognition of its capabilities and have essentially assisted the development of commercial instruments. For many significant applications, such instruments provide reliable measurements of spherical particles of known refractive index and diameters exceeding about 5 µm.…”
Section: Introductionmentioning
confidence: 99%
“…The principles of phase-Doppler anemometry for determining simultaneously velocity and size distributions of suspended spherical particles were first presented by Durst and Zaré [1]. Subsequent contributions to the development of phase-Doppler anemometry, for example [2][3][4] were essential to the development of the technique and the recognition of its capabilities and have essentially assisted the development of commercial instruments. For many significant applications, such instruments provide reliable measurements of spherical particles of known refractive index and diameters exceeding about 5 µm.…”
Section: Introductionmentioning
confidence: 99%
“…For non-intrusive and simultaneous measurements of particle velocity and particle size, phase-Doppler anemometry is a very suitable method (Buuckhuge and Flogel [l], Saffmun et al [2], Buchalo and Houser [3], referring to fundamentals described by Durst and ZurP [4]). This measuring technique yields absolute results of particle size and velocity, but in the case of the prevailing application, i. e. the analysis of multi-phase flows with polydisperse particle collections (Buchalo and Houser [5], Bauckhuge [6], Bauckhuge et al [7]), the measured number distributions of particles sizes are biased in a way that large particles are over-represented in comparison with smaller ones ([2], Bauckhuge et al [8], Suffman [9], Bachulo [lo]). Therefore, a weighting procedure becomes necessary to obtain correct results for the corresponding distributions and for all related flow parameters, such as particle concentration and mass flux density.…”
Section: Introductionmentioning
confidence: 99%
“…The commonly used function for weighting size distributions is the area of detection, being part of the cross-sectional area of the measuring volume. If reflecting particles are measured with the aid of a backscatter PDA, the size of the detection area can be determined very easily value of burst amplitudes (Sommerfeld and Qiu [12]), the maximum burst length, the maximum number of signal periods above a fixed trigger level [8,101 or the mean value of squared burst lengths 191. For a specific weighting procedure, either the burst, generated by only one reference particle with well known diameter do, moving through the centre of the measuring volume, or the bursts of single reference particles in each particle size class di, have to be analysed with respect to their lengths or amplitudes.…”
Section: Introductionmentioning
confidence: 99%