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  <title><![CDATA[Toward a Precise Continuum Model for Dense Granular Flows]]></title>
  <body><![CDATA[<h5>School of Physics Soft Condensed Matter and Biophysics Seminar: Presenting&nbsp;Ken Kamrin, MIT</h5><p>The challenge of predicting velocity and stress fields in any flowing granular material has proven to be a difficult one, from both computational and theoretical perspectives.&nbsp; Indeed, researchers are still in search of the ``Navier-Stokes"-equivalent for flowing granular materials.&nbsp;&nbsp; Granular flows can be adequately predicted using grain-by-grain discrete element methods (DEM), but these approaches become computationally unrealistic for large bodies of material and long times.&nbsp;&nbsp; A robust continuum model, once identified, would have the practical benefit that it could be implemented at a meso-scale saving many orders of magnitude in computation time compared to DEM.</p><p>Here, we begin by synthesizing a 3D elasto-viscoplastic law for steady granular flow, merging an existing "frictional fluid" relation with a nonlinear granular elasticity relation to close the system.&nbsp; The flow rate vanishes within a frictional (Drucker-Prager) yield surface and the elastic response is based on a mean-field model generalizing Hertz's contact law. The resulting form is general, able to produce flow and stress predictions&nbsp; in any well-posed boundary value problem.&nbsp; We implement it using ABAQUS/Explicit finite-element package and run test simulations in multiple geometries. The solutions are shown to compare favorably against a number of experiments and DEM simulations.</p><p>While this relation appears to function well for rapid flows, experimental results can often differ from the predictions in regions of slower flows.&nbsp; We have been able to attribute many of these phenomena to nonlocal effects stemming from the finite-ness of the grain size.&nbsp; To correct this, we consider the addition of a simple nonlocal term to the rheology in a fashion similar to recent nonlocal flow models in the emulsions community.&nbsp; The results of this extended model are compared against many DEM steady-flow simulations in three different 2D geometries.&nbsp; Quantitative agreement is found for all geometries and over various geometrical/loading parameters.&nbsp; By natural extension, the nonlocal model is then converted to three dimensions with minimal changes, and is implemented numerically as a User-Element in the ABAQUS package.&nbsp; We show that a single calibration of the 3D model quantitatively predicts hundreds of experimental flows in different geometries, including, for the first time, the wide-shear zones observed in the split-bottom annular couette cell, a geometry made infamous for resisting a theoretical treatment for almost a decade.</p><p>&nbsp;</p>]]></body>
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      <value><![CDATA[2012-10-16T16:00:00-04:00]]></value>
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      <timezone><![CDATA[America/New_York]]></timezone>
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      <value><![CDATA[free]]></value>
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      <value><![CDATA[<p><a href="mailto:alison.morain@physics.gatech.edu">alison.morain@physics.gatech.edu</a></p>]]></value>
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      <value><![CDATA[(404) 894-8886]]></value>
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      <url><![CDATA[https://www.physics.gatech.edu/seminars-colloquia/series/soft-condensed-matter-and-biophysics/ken-kamrin-20121016]]></url>
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        <url>http://web.mit.edu/kkamrin/www/</url>
        <link_title><![CDATA[http://web.mit.edu/kkamrin/www/]]></link_title>
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        <url>https://www.physics.gatech.edu/seminars-colloquia/series/soft-condensed-matter-and-biophysics/ken-kamrin-20121016</url>
        <link_title><![CDATA[https://www.physics.gatech.edu/seminars-colloquia/series/soft-condensed-mat...]]></link_title>
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