{"title":"Arrêt d'un écoulement granulaire sur une pente faible","authors":"Thomas Boutreux, Pierre-Gilles de Gennes","doi":"10.1016/S1251-8069(98)80035-3","DOIUrl":null,"url":null,"abstract":"<div><p>A ridge of sand, with initial angles ± θ<sub>i</sub> (smaller than the angle of repose θ<sub>r</sub>) is fed by a source of flux 2Q. We discuss here the theoretical profile achieved after a time t, using the equations of Bouchaud et al. in their original form, and also in a modified form which might apply for strong flows. The result is a central heap, steeper than the original ridge, of slope close to θ<sub>r</sub>. The horizontal span is predicted to be x<sub>m</sub> = (2Dt)<sup>1/2</sup>, with an apparent diffusion coefficient D = Q/(θ<sub>r</sub> − θ<sub>i</sub>).</p></div>","PeriodicalId":100304,"journal":{"name":"Comptes Rendus de l'Académie des Sciences - Series IIB - Mechanics-Physics-Chemistry-Astronomy","volume":"326 4","pages":"Pages 257-262"},"PeriodicalIF":0.0000,"publicationDate":"1998-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S1251-8069(98)80035-3","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Comptes Rendus de l'Académie des Sciences - Series IIB - Mechanics-Physics-Chemistry-Astronomy","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1251806998800353","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
A ridge of sand, with initial angles ± θi (smaller than the angle of repose θr) is fed by a source of flux 2Q. We discuss here the theoretical profile achieved after a time t, using the equations of Bouchaud et al. in their original form, and also in a modified form which might apply for strong flows. The result is a central heap, steeper than the original ridge, of slope close to θr. The horizontal span is predicted to be xm = (2Dt)1/2, with an apparent diffusion coefficient D = Q/(θr − θi).