1985
DOI: 10.1029/jd090id06p10620
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A volcanic ash transport model and analysis of Mount St. Helens ashfall

Abstract: A model is presented to compute the transport and deposition of volcanic ash particles. Calculations use variable winds along the particle trajectories. The model was exercised by performing numerical experiments with data from the May 18, 1980, eruption of Mount St. Helens, Washington. Ashfall arrival times, location of grounded ash, a particle size distribution, and particle size sorting across the grounded ash lobes were calculated and compared to observations. Agreement was generally found, except for the … Show more

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Cited by 18 publications
(12 citation statements)
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“…The resultant airfall deposit had a second thickness maximum located 350 km from the volcano. Carey & Sigurdsson (1982), supported by Hopkins & Bridgman (1985), concluded the Mount St Helens thickening resulted from the aerial aggregation of fine ash particles (<63 |im) followed by the premature fallout of the aggregates. The resultant terrestrial deposit tended to be fine grained, polymodal, and poorly sorted.…”
Section: Onshore Versus Offshore Dispersalmentioning
confidence: 83%
“…The resultant airfall deposit had a second thickness maximum located 350 km from the volcano. Carey & Sigurdsson (1982), supported by Hopkins & Bridgman (1985), concluded the Mount St Helens thickening resulted from the aerial aggregation of fine ash particles (<63 |im) followed by the premature fallout of the aggregates. The resultant terrestrial deposit tended to be fine grained, polymodal, and poorly sorted.…”
Section: Onshore Versus Offshore Dispersalmentioning
confidence: 83%
“…It is assumed that the terms related to transport by diffusion processes are negligible, that the plume is maintained and long-lived (steady), and that motion of the carrying medium (eruption column, umbrella cloud or downwind plume) can be characterized by a single coordinate at University of Iowa on June 28, 2015 http://sp.lyellcollection.org/ Downloaded from direction s-for which the axis is everywhere tangent to the plume centreline (e.g. Wright 1977;Hopkins & Bridgman 1985) -and speed U in that direction. Under these assumptions, equation (7) …”
Section: Pyroclast Falloutmentioning
confidence: 99%
“…Atmospheric motions can then be simulated by using the summation or superposition of waves of progressively higher wavenumber (shorter wavelength) (e.g. Saucier 1983;Hopkins & Bridgman 1985;Pedlosky 1987) with kinetic energies (velocities) dependent on wavenumber, for example (simplifying from Behringer et al 1991; see also Hopkins & Bridgman 1985) z~ = Z urn(sin(k,,x + ~,,,t ) DI + sin(krny + ~rnt))…”
Section: Distal Transport Of Volcanic Eruption Productsmentioning
confidence: 99%
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“…The approach is based on the attempt to formulate equations (balance of mass, of momentum, of energy, laws of state) that simulate eruption behavior [3][4][5][6][7]. The system of equations is then solved via numerical methods.…”
Section: Simulation Models and Hazard Mappingmentioning
confidence: 99%