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      <ref-type name="Journal Article">17</ref-type>
      <work-type>ACL : Articles dans des revues avec comité de lecture répertoriées par l'AERES</work-type>
      <contributors>
        <authors>
          <author>
            <style face="bold" font="default" size="100%">Roche, Olivier</style>
          </author>
          <author>
            <style face="normal" font="default" size="100%">Montserrat, S.</style>
          </author>
          <author>
            <style face="normal" font="default" size="100%">Nino, Y.</style>
          </author>
          <author>
            <style face="normal" font="default" size="100%">Tamburrino, A.</style>
          </author>
        </authors>
      </contributors>
      <titles>
        <title>Experimental observations of water-like behavior of initially fluidized, dam break granular flows and their relevance for the propagation of ash-rich pyroclastic flows</title>
        <secondary-title>Journal of Geophysical Research - Solid Earth</secondary-title>
      </titles>
      <pages>B12203</pages>
      <dates>
        <year>2008</year>
      </dates>
      <call-num>fdi:010046767</call-num>
      <language>ENG</language>
      <periodical>
        <full-title>Journal of Geophysical Research - Solid Earth</full-title>
      </periodical>
      <isbn>0148-0227</isbn>
      <accession-num>ISI:000261687700002</accession-num>
      <number>B12</number>
      <electronic-resource-num>10.1029/2008jb005664</electronic-resource-num>
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          <url>https://www.documentation.ird.fr/hor/fdi:010046767</url>
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          <url>https://www.documentation.ird.fr/intranet/publi/depot/2009-07-01/010046767.pdf</url>
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      <volume>113</volume>
      <remote-database-provider>Horizon (IRD)</remote-database-provider>
      <abstract>The physics of ash-rich pyroclastic flows were investigated through laboratory dam break experiments using both granular material and water. Flows of glass beads of 60-90 mu m in diameter generated from the release of initially fluidized, slightly expanded (2.5-4.5%) columns behave as their inertial water counterparts for most of their emplacement. For a range of initial column height to length ratios of 0.5-3, both types of flows propagate in three stages, controlled by the time scale of column free fall similar to(h(0)/g)(1/2), where h(0) denotes column height and g denotes gravitational acceleration. Flows first accelerate as the column collapses. Transition to a second, constant velocity phase occurs at a time t/(h(0)/g)(1/2) similar to 1.5. The flow velocity is then U similar to root 2(gh(0))(1/2), larger than that for dry (initially nonfluidized) granular flows. Transition to a last, third phase occurs at t/(h(0)/g)(1/2) similar to 4. Granular flow behavior then departs from that of water flows as the former steadily decelerates and the front position varies as t(1/3), as in dry flows. Motion ceases at t/(h(0)/g) 1/2 similar to 6.5 with normalized runout x/h(0) similar to 5.5-6. The equivalent behavior of water and highly concentrated granular flows up to the end of the second phase indicates a similar overall bulk resistance, although mechanisms of energy dissipation in both cases would be different. Interstitial air-particle viscous interactions can be dominant and generate pore fluid pressure sufficient to confer a fluid-inertial behavior to the dense granular flows before they enter a granular-frictional regime at late stages. Efficient gas-particle interactions in dense, ash-rich pyroclastic flows may promote a water-like behavior during most of their propagation.</abstract>
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      <custom7>Chili</custom7>
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