Three-dimensional turbulent velocity field and air entrainment of the 22 March 1944 Vesuvius eruption plume

被引:0
|
作者
Andrews, Benjamin J. [1 ]
Coonin, Allie N. [2 ]
机构
[1] Smithsonian Inst, Natl Museum Nat Hist, Global Volcanism Program, Washington, DC 20560 USA
[2] Brown Univ, Dept Earth Environm & Planetary Sci, Providence, RI 02912 USA
基金
美国国家科学基金会;
关键词
Plinian eruption; Turbulence; Air entrainment; Image analysis; Plume dynamics; MOUNT ST-HELENS; VOLCANIC PLUMES; LABORATORY EXPERIMENTS; DYNAMICS; MODEL; WIND; THERMODYNAMICS; SIMULATION; PARAMETERS; TRANSPORT;
D O I
10.1007/s00445-024-01703-1
中图分类号
P [天文学、地球科学];
学科分类号
07 ;
摘要
Turbulent air entrainment into explosive volcanic jets determines whether an eruption will produce buoyant plumes, pyroclastic density currents, or both. Most previous studies of entrainment consist of numerical models and analog laboratory experiments, with relatively few observations of natural eruptions. The existing observations of entrainment are generally time- and space-averaged measurements, which do not provide information regarding the mechanisms of entrainment. We investigate spatial and temporal variations in entrainment of the March 22 Plinian phase of the 1944 eruption of Mt. Vesuvius using a feature tracking velocimetry (FTV) algorithm applied to film collected by the U.S. Navy and digitized by the U.S. National Archives. We describe a novel technique to estimate the 3D plume morphology from normalized brightness. Projection of the 2D velocity fields from the FTV algorithm onto those 3D surfaces provides 3D velocity fields. The divergence of the velocity fields quantifies local expansion and entrainment and shows that although kilometer scale eddies are present in the plume, entrainment and expansion occur over length scales on the order of hundreds of meters. Integrating the inward directed velocities over the entraining regions quantifies local air entrainment rates. We find that entrainment of 5.4-6.1 x 10(7) m(3)s(-1) air occurs over about one-third of the observed plume margins, yielding an average entrainment velocity of similar to 2.8 ms(-1). Extrapolation of those rates to the entire plume indicates total entrainment of 1-3 x 10(8) m(3)s(-1). The entrainment velocity has a magnitude similar to 6% of the magnitude of the turbulence intensity along the plume margins, indicating that the latter may approximate the centerline plume velocity and suggesting use of entrainment coefficient of 0.06 for this and similar eruptions, i.e., strong plumes with a relatively high momentum-dominated region.
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页数:15
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