2004
DOI: 10.1029/2003jb002388
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Reply to comment by C. Textor and G. G. J. Ernst on“Particle aggregation in volcanic eruption columns”

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Cited by 3 publications
(2 citation statements)
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“…The settling velocity of nonspherical particles is also allowed to vary as a function of height above the ground due to major variations in air density and viscosity with altitude [ Wilson , 1972]. In contrast, particle aggregation processes are not described by the present model, although they can play a major role in some conditions [ Textor and Ernst , 2004; Veitch and Woods , 2004].…”
Section: The Vol‐calpuff Codementioning
confidence: 99%
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“…The settling velocity of nonspherical particles is also allowed to vary as a function of height above the ground due to major variations in air density and viscosity with altitude [ Wilson , 1972]. In contrast, particle aggregation processes are not described by the present model, although they can play a major role in some conditions [ Textor and Ernst , 2004; Veitch and Woods , 2004].…”
Section: The Vol‐calpuff Codementioning
confidence: 99%
“…Later on, the equation sets of these so‐called “plume theory” models were integrated by adding the energy conservation equation in different forms [ Woods , 1988; Glaze and Baloga , 1996]. Further developments concerned the modeling of thermal disequilibrium [ Woods and Bursik , 1991], particle fallout from the column [ Woods and Bursik , 1991; Ernst et al , 1996], and umbrella cloud [ Bursik et al , 1992b; Bonadonna et al , 1998], and particle recycling into the eruption column [ Ernst et al , 1996; Veitch and Woods , 2002, 2004; Textor et al , 2004]. Crosswind influence on plume tilting has also been addressed based on experimental and theoretical work on turbulent buoyant plumes in cross flow [ Hoult and Weil , 1972; Wright , 1984; Ernst et al , 1994; Bursik , 2001].…”
Section: Introductionmentioning
confidence: 99%