Hindered flotation functions from nuclear magnetic resonance imaging

In batch settling or flotation the velocity of the disperse phase u d =U S G(φ). U S is the terminal velocity of an isolated particle, and G is the hindrance function. Vertical profiles of the fluid fraction in batch flotation experiments, measured by one-dimensional nuclear magnetic resonance (NMR)...

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Veröffentlicht in:Journal of rheology (New York : 1978) 2002-11, Vol.46 (6), p.1341-1352
Hauptverfasser: Altobelli, Stephen A., Mondy, Lisa A.
Format: Artikel
Sprache:eng
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Zusammenfassung:In batch settling or flotation the velocity of the disperse phase u d =U S G(φ). U S is the terminal velocity of an isolated particle, and G is the hindrance function. Vertical profiles of the fluid fraction in batch flotation experiments, measured by one-dimensional nuclear magnetic resonance (NMR) imaging, were input into a new method for extracting G. This simple, explicit calculation was tested on concentrated monodisperse and polydisperse samples. In a single experiment on a 44 mL sample of monodisperse suspension with overall solid fraction φ i =0.2, the hindered flotation function G(φ) was measured over the range of 0.05 
ISSN:0148-6055
1520-8516
DOI:10.1122/1.1514199