Numerical modeling of avalanches based on Saint Venant equations using a kinetic scheme
Numerical modeling of debris avalanche is presented here. The model uses the long‐wave approximation based on the small aspect ratio of debris avalanches as in classical Saint Venant model of shallow water. Depth‐averaged equations using this approximation are derived in a reference frame linked to...
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Veröffentlicht in: | Journal of Geophysical Research 2003-11, Vol.108 (B11), p.EPM9.1-n/a |
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description | Numerical modeling of debris avalanche is presented here. The model uses the long‐wave approximation based on the small aspect ratio of debris avalanches as in classical Saint Venant model of shallow water. Depth‐averaged equations using this approximation are derived in a reference frame linked to the topography. Debris avalanche is treated here as a single‐phase, dry granular flow with Coulomb‐type behavior. The numerical finite volume method uses a kinetic scheme based on the description of the microscopic behavior of the system to define numerical fluxes at the interfaces of a finite element mesh. The main advantage of this method is to preserve the height positivity. The originality of the presented scheme stands in the introduction of a Dirac distribution of particles at the microscopic scale in order to describe the stopping of a granular mass when the driving forces are under the Coulomb threshold. Comparisons with analytical solutions for dam break problems and experimental results show the efficiency of the model in dealing with significant discontinuities and reproducing the flowing and stopping phase of granular avalanches. The ability of the model to describe debris avalanche behavior is illustrated here by schematic numerical simulation of an avalanche over simplified topography. Coulomb‐type behavior with constant and variable friction angle is compared in the framework of this simple example. Numerical tests show that such an approach not only provides insights into the flowing and stopping stage of the granular mass but allows observation of interesting behavior such as the existence of a fluid‐like zone behind a stopped solid‐like granular mass in specific situations, suggesting the presence of horizontal surfaces in the deposited mass. |
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O. ; Perthame, B. ; Bouchut, F. ; Simeoni, C. ; Yerneni, S.</creator><creatorcontrib>Mangeney-Castelnau, A. ; Vilotte, J.-P. ; Bristeau, M. O. ; Perthame, B. ; Bouchut, F. ; Simeoni, C. ; Yerneni, S.</creatorcontrib><description>Numerical modeling of debris avalanche is presented here. The model uses the long‐wave approximation based on the small aspect ratio of debris avalanches as in classical Saint Venant model of shallow water. Depth‐averaged equations using this approximation are derived in a reference frame linked to the topography. Debris avalanche is treated here as a single‐phase, dry granular flow with Coulomb‐type behavior. The numerical finite volume method uses a kinetic scheme based on the description of the microscopic behavior of the system to define numerical fluxes at the interfaces of a finite element mesh. The main advantage of this method is to preserve the height positivity. The originality of the presented scheme stands in the introduction of a Dirac distribution of particles at the microscopic scale in order to describe the stopping of a granular mass when the driving forces are under the Coulomb threshold. Comparisons with analytical solutions for dam break problems and experimental results show the efficiency of the model in dealing with significant discontinuities and reproducing the flowing and stopping phase of granular avalanches. The ability of the model to describe debris avalanche behavior is illustrated here by schematic numerical simulation of an avalanche over simplified topography. Coulomb‐type behavior with constant and variable friction angle is compared in the framework of this simple example. Numerical tests show that such an approach not only provides insights into the flowing and stopping stage of the granular mass but allows observation of interesting behavior such as the existence of a fluid‐like zone behind a stopped solid‐like granular mass in specific situations, suggesting the presence of horizontal surfaces in the deposited mass.</description><identifier>ISSN: 0148-0227</identifier><identifier>EISSN: 2156-2202</identifier><identifier>DOI: 10.1029/2002JB002024</identifier><language>eng</language><publisher>Washington, DC: Blackwell Publishing Ltd</publisher><subject>avalanche modeling ; Computer Science ; Coulomb friction ; Earth Sciences ; Earth, ocean, space ; Engineering and environment geology. Geothermics ; Engineering geology ; Engineering Sciences ; Exact sciences and technology ; finite volume kinetic scheme ; Fluids mechanics ; Geophysics ; gravitational flow ; Mathematics ; Mechanics ; Modeling and Simulation ; Natural hazards: prediction, damages, etc ; Numerical Analysis ; Saint Venant equations ; Sciences of the Universe</subject><ispartof>Journal of Geophysical Research, 2003-11, Vol.108 (B11), p.EPM9.1-n/a</ispartof><rights>Copyright 2003 by the American Geophysical Union.</rights><rights>2004 INIST-CNRS</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a5999-9bc33aada3b8f56c9a1e100868a66175f6bfc3651ecc9302d874641f82db5be3</citedby><cites>FETCH-LOGICAL-a5999-9bc33aada3b8f56c9a1e100868a66175f6bfc3651ecc9302d874641f82db5be3</cites><orcidid>0000-0002-6085-6498 ; 0000-0002-7733-4645 ; 0000-0002-2545-1655 ; 0000-0002-7091-1200</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2002JB002024$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2002JB002024$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>230,314,777,781,882,1412,1428,11495,27905,27906,45555,45556,46390,46449,46814,46873</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=15392223$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-00922781$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Mangeney-Castelnau, A.</creatorcontrib><creatorcontrib>Vilotte, J.-P.</creatorcontrib><creatorcontrib>Bristeau, M. O.</creatorcontrib><creatorcontrib>Perthame, B.</creatorcontrib><creatorcontrib>Bouchut, F.</creatorcontrib><creatorcontrib>Simeoni, C.</creatorcontrib><creatorcontrib>Yerneni, S.</creatorcontrib><title>Numerical modeling of avalanches based on Saint Venant equations using a kinetic scheme</title><title>Journal of Geophysical Research</title><addtitle>J. Geophys. Res</addtitle><description>Numerical modeling of debris avalanche is presented here. The model uses the long‐wave approximation based on the small aspect ratio of debris avalanches as in classical Saint Venant model of shallow water. Depth‐averaged equations using this approximation are derived in a reference frame linked to the topography. Debris avalanche is treated here as a single‐phase, dry granular flow with Coulomb‐type behavior. The numerical finite volume method uses a kinetic scheme based on the description of the microscopic behavior of the system to define numerical fluxes at the interfaces of a finite element mesh. The main advantage of this method is to preserve the height positivity. The originality of the presented scheme stands in the introduction of a Dirac distribution of particles at the microscopic scale in order to describe the stopping of a granular mass when the driving forces are under the Coulomb threshold. Comparisons with analytical solutions for dam break problems and experimental results show the efficiency of the model in dealing with significant discontinuities and reproducing the flowing and stopping phase of granular avalanches. The ability of the model to describe debris avalanche behavior is illustrated here by schematic numerical simulation of an avalanche over simplified topography. Coulomb‐type behavior with constant and variable friction angle is compared in the framework of this simple example. Numerical tests show that such an approach not only provides insights into the flowing and stopping stage of the granular mass but allows observation of interesting behavior such as the existence of a fluid‐like zone behind a stopped solid‐like granular mass in specific situations, suggesting the presence of horizontal surfaces in the deposited mass.</description><subject>avalanche modeling</subject><subject>Computer Science</subject><subject>Coulomb friction</subject><subject>Earth Sciences</subject><subject>Earth, ocean, space</subject><subject>Engineering and environment geology. Geothermics</subject><subject>Engineering geology</subject><subject>Engineering Sciences</subject><subject>Exact sciences and technology</subject><subject>finite volume kinetic scheme</subject><subject>Fluids mechanics</subject><subject>Geophysics</subject><subject>gravitational flow</subject><subject>Mathematics</subject><subject>Mechanics</subject><subject>Modeling and Simulation</subject><subject>Natural hazards: prediction, damages, etc</subject><subject>Numerical Analysis</subject><subject>Saint Venant equations</subject><subject>Sciences of the Universe</subject><issn>0148-0227</issn><issn>2156-2202</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNqNkc1u1DAUhS0EEqPSHQ_gDUhIBK7t2LGXnRFMGY0GqYzo0rpxHGqanzZOCn17HKUqrAAvfGXrO0f36BDyksE7Bty85wB8t04X8PwJWXEmVcbT4ylZAct1BpwXz8lpjN8hnVyqHNiKXB6m1g_BYUPbvvJN6L7RvqZ4hw127spHWmL0Fe07-gVDN9KvvsM0_O2EY-i7SKc4a5Beh86PwdGYVK1_QZ7V2ER_-jBPyPHjh-PmPNt_3n7anO0zlMaYzJROCMQKRalrqZxB5hmAVhqVYoWsVVk7oSTzzhkBvNJFrnJWa16VsvTihLxZbK-wsTdDaHG4tz0Ge362t_MfgEm5NbtjiX29sDdDfzv5ONo2ROebFNT3U7QJMyDA_A-odcH_DTLDtAA9g28X0A19jIOvH3dlYOf27J_tJfzVgy_G1Ew9pCpC_K2RIoXiInFi4X6Ext__1dPuthdrJmQ-L5MtqhBH__NRhcO1VYUopL08bO3meLHebTcHW4hf_2S1Mg</recordid><startdate>200311</startdate><enddate>200311</enddate><creator>Mangeney-Castelnau, A.</creator><creator>Vilotte, J.-P.</creator><creator>Bristeau, M. 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O. ; Perthame, B. ; Bouchut, F. ; Simeoni, C. ; Yerneni, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a5999-9bc33aada3b8f56c9a1e100868a66175f6bfc3651ecc9302d874641f82db5be3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>avalanche modeling</topic><topic>Computer Science</topic><topic>Coulomb friction</topic><topic>Earth Sciences</topic><topic>Earth, ocean, space</topic><topic>Engineering and environment geology. 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The numerical finite volume method uses a kinetic scheme based on the description of the microscopic behavior of the system to define numerical fluxes at the interfaces of a finite element mesh. The main advantage of this method is to preserve the height positivity. The originality of the presented scheme stands in the introduction of a Dirac distribution of particles at the microscopic scale in order to describe the stopping of a granular mass when the driving forces are under the Coulomb threshold. Comparisons with analytical solutions for dam break problems and experimental results show the efficiency of the model in dealing with significant discontinuities and reproducing the flowing and stopping phase of granular avalanches. The ability of the model to describe debris avalanche behavior is illustrated here by schematic numerical simulation of an avalanche over simplified topography. Coulomb‐type behavior with constant and variable friction angle is compared in the framework of this simple example. Numerical tests show that such an approach not only provides insights into the flowing and stopping stage of the granular mass but allows observation of interesting behavior such as the existence of a fluid‐like zone behind a stopped solid‐like granular mass in specific situations, suggesting the presence of horizontal surfaces in the deposited mass.</abstract><cop>Washington, DC</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2002JB002024</doi><tpages>18</tpages><orcidid>https://orcid.org/0000-0002-6085-6498</orcidid><orcidid>https://orcid.org/0000-0002-7733-4645</orcidid><orcidid>https://orcid.org/0000-0002-2545-1655</orcidid><orcidid>https://orcid.org/0000-0002-7091-1200</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | avalanche modeling Computer Science Coulomb friction Earth Sciences Earth, ocean, space Engineering and environment geology. Geothermics Engineering geology Engineering Sciences Exact sciences and technology finite volume kinetic scheme Fluids mechanics Geophysics gravitational flow Mathematics Mechanics Modeling and Simulation Natural hazards: prediction, damages, etc Numerical Analysis Saint Venant equations Sciences of the Universe |
title | Numerical modeling of avalanches based on Saint Venant equations using a kinetic scheme |
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