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	<journal>
		<journal_title>Solid Earth Discussions</journal_title>
		<journal_url>www.solid-earth-discuss.net</journal_url>
		<eissn>1869-9537</eissn>
		<volume_number>4</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2012</publication_year>
	</journal>
	<doi>10.5194/sed-4-173-2012</doi>
	<article_url>http://www.solid-earth-discuss.net/4/173/2012/</article_url>
	<abstract_html>http://www.solid-earth-discuss.net/4/173/2012/sed-4-173-2012.html</abstract_html>
	<fulltext_pdf>http://www.solid-earth-discuss.net/4/173/2012/sed-4-173-2012.pdf</fulltext_pdf>
	<start_page>173</start_page>
	<end_page>202</end_page>
	<publication_date>2012-01-26</publication_date>
	<article_title content_type="html">New developments in the analysis of volcanic pyroclastic density currents through numerical simulations of multiphase flows</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>S. Lepore</name>
			<email>simone.lepore@unina.it</email>
		</author>
		<author numeration="2" affiliations="1">
			<name>C. Scarpati</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Dipartimento di Scienze della Terra, University of Naples Federico II, Largo San Marcellino 10, 80138 &amp;ndash; Naples, Italy</affiliation>
	</affiliations>
	<abstract content_type="html">A granular multiphase model has been used to evaluate the action of
differently sized particles on the dynamics of fountains and associated
pyroclastic density currents. The model takes into account the overall
disequilibrium conditions between a gas phase and several solid phases, each
characterized by its own physical properties. The dynamics of the granular
flows has been simulated by adopting a Reynolds Average Navier-Stokes
model for describing the turbulence effects. Numerical simulations have been
carried out by using different values for the eruptive column temperature at
the vent, solid particles frictional concentration, turbulent kinetic
energy, and dissipation. The results obtained underline the importance of
the multiphase nature of the model and characterize several disequilibrium
effects. The low concentration (&amp;le; 5 &amp;middot; 10&lt;sup&gt;&amp;ndash;4&lt;/sup&gt;) sectors lie in
the upper part of the granular flow, above the fountain, and above the
pyroclastic current tail and body as thermal plumes. The high concentration
sectors, on the contrary, form the fountain and remain along the ground of
the granular flow. Hence, pyroclastic density currents are assimilated to
granular flows constituted by a low concentration suspension flowing above a
high concentration basal layer (boundary layer), from the proximal regions
to the distal ones. Interactions among solid, differently sized particles in
the boundary layer of the granular flow are controlled by collisions between
particles, whereas particles dispersal in the suspension is determined by
the dragging of the gas phase. The simulations describe well the dynamics of
a tractive boundary layer leading to the formation of stratified facies
during eruptions having a different magnitude.</abstract>
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</article>

