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 |
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Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
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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 |
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ISSN: | 0148-6055 1520-8516 |
DOI: | 10.1122/1.1514199 |