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The effect of particle shape on discharge and clogging

Granular flow is common across different fields from energy resource recovery and mineral processing to grain transport and traffic flow. Migrating particles may jam and form arches that span constrictions and hinder particle flow. Most studies have investigated the migration and clogging of spheric...

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Autores principales: Hafez, Ahmed, Liu, Qi, Finkbeiner, Thomas, Alouhali, Raed A., Moellendick, Timothy E., Santamarina, J. Carlos
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7870973/
https://www.ncbi.nlm.nih.gov/pubmed/33558548
http://dx.doi.org/10.1038/s41598-021-82744-w
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author Hafez, Ahmed
Liu, Qi
Finkbeiner, Thomas
Alouhali, Raed A.
Moellendick, Timothy E.
Santamarina, J. Carlos
author_facet Hafez, Ahmed
Liu, Qi
Finkbeiner, Thomas
Alouhali, Raed A.
Moellendick, Timothy E.
Santamarina, J. Carlos
author_sort Hafez, Ahmed
collection PubMed
description Granular flow is common across different fields from energy resource recovery and mineral processing to grain transport and traffic flow. Migrating particles may jam and form arches that span constrictions and hinder particle flow. Most studies have investigated the migration and clogging of spherical particles, however, natural particles are rarely spherical, but exhibit eccentricity, angularity and roughness. New experiments explore the discharge of cubes, 2D crosses, 3D crosses and spheres under dry conditions and during particle-laden fluid flow. Variables include orifice-to-particle size ratio and solidity. Cubes and 3D crosses are the most prone to clogging because of their ability to interlock or the development of face-to-face contacts that can resist torque and enhance bridging. Spheres arriving to the orifice must be correctly positioned to create stable bridges, while flat 2D crosses orient their longest axes in the direction of flowlines across the orifice and favor flow. Intermittent clogging causes kinetic retardation in particle-laden flow even in the absence of inertial effects; the gradual increase in the local particle solidity above the constriction enhances particle interactions and the probability of clogging. The discharge volume before clogging is a Poisson process for small orifice-to-particle size ratio; however, the clogging probability becomes history-dependent for non-spherical particles at large orifice-to-particle size ratio and high solidities, i.e., when particle–particle interactions and interlocking gain significance.
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spelling pubmed-78709732021-02-10 The effect of particle shape on discharge and clogging Hafez, Ahmed Liu, Qi Finkbeiner, Thomas Alouhali, Raed A. Moellendick, Timothy E. Santamarina, J. Carlos Sci Rep Article Granular flow is common across different fields from energy resource recovery and mineral processing to grain transport and traffic flow. Migrating particles may jam and form arches that span constrictions and hinder particle flow. Most studies have investigated the migration and clogging of spherical particles, however, natural particles are rarely spherical, but exhibit eccentricity, angularity and roughness. New experiments explore the discharge of cubes, 2D crosses, 3D crosses and spheres under dry conditions and during particle-laden fluid flow. Variables include orifice-to-particle size ratio and solidity. Cubes and 3D crosses are the most prone to clogging because of their ability to interlock or the development of face-to-face contacts that can resist torque and enhance bridging. Spheres arriving to the orifice must be correctly positioned to create stable bridges, while flat 2D crosses orient their longest axes in the direction of flowlines across the orifice and favor flow. Intermittent clogging causes kinetic retardation in particle-laden flow even in the absence of inertial effects; the gradual increase in the local particle solidity above the constriction enhances particle interactions and the probability of clogging. The discharge volume before clogging is a Poisson process for small orifice-to-particle size ratio; however, the clogging probability becomes history-dependent for non-spherical particles at large orifice-to-particle size ratio and high solidities, i.e., when particle–particle interactions and interlocking gain significance. Nature Publishing Group UK 2021-02-08 /pmc/articles/PMC7870973/ /pubmed/33558548 http://dx.doi.org/10.1038/s41598-021-82744-w Text en © The Author(s) 2021 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Hafez, Ahmed
Liu, Qi
Finkbeiner, Thomas
Alouhali, Raed A.
Moellendick, Timothy E.
Santamarina, J. Carlos
The effect of particle shape on discharge and clogging
title The effect of particle shape on discharge and clogging
title_full The effect of particle shape on discharge and clogging
title_fullStr The effect of particle shape on discharge and clogging
title_full_unstemmed The effect of particle shape on discharge and clogging
title_short The effect of particle shape on discharge and clogging
title_sort effect of particle shape on discharge and clogging
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7870973/
https://www.ncbi.nlm.nih.gov/pubmed/33558548
http://dx.doi.org/10.1038/s41598-021-82744-w
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