Multifluid flow in bedded porous media: laboratory experiments and numerical simulations
Understanding light nonaqueous-phase liquid (LNAPL) movement in heterogeneous vadose environments is important for effective remediation design. We investigated LNAPL movement near a sloping fine- over coarse-grained textural interface, forming a capillary barrier. LNAPL flow experiments were perfor...
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creator | Schroth, M.H. Istok, J.D. Selker, J.S. Oostrom, M. White, M.D. |
description | Understanding light nonaqueous-phase liquid (LNAPL) movement in heterogeneous vadose environments is important for effective remediation design. We investigated LNAPL movement near a sloping fine- over coarse-grained textural interface, forming a capillary barrier. LNAPL flow experiments were performed in a glass chamber (50
cm×60
cm×1.0
cm) using two silica sands (12/20 and 30/40 sieve sizes). Variable water saturations near the textural interface were generated by applying water uniformly to the sand surface at various flow rates. A model LNAPL (Soltrol® 220) was subsequently released at two locations at the sand surface. Visible light transmission was used to quantitatively determine water saturations prior to LNAPL release and to observe LNAPL flow paths. Numerical simulations were performed using the Subsurface Transport Over Multiple Phases (STOMP) simulator, employing two nonhysteretic relative permeability–saturation–pressure (
k–
S–
P) models. LNAPL movement strongly depended on the water saturation in the fine-grained sand layer above the textural interface. In general, reasonable agreement was found between observed and predicted water saturations near the textural interface and LNAPL flow paths. Discrepancies between predictions based on the van Genuchten/Mualem (VGM) and Brooks–Corey/Burdine (BCB)
k–
S–
P models existed in the migration speed of the simulated LNAPL plume and the LNAPL flow patterns at high water saturation above the textural interface. In both instances, predictions based on the BCB model agreed better with experimental observations than predictions based on the VGM model. The results confirm the critical role water saturation plays in determining LNAPL movement in heterogeneous vadose zone environments and that accurate prediction of LNAPL flow paths depends on the careful selection of an appropriate
k–
S–
P model. |
doi_str_mv | 10.1016/S0309-1708(97)00043-2 |
format | Article |
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cm×60
cm×1.0
cm) using two silica sands (12/20 and 30/40 sieve sizes). Variable water saturations near the textural interface were generated by applying water uniformly to the sand surface at various flow rates. A model LNAPL (Soltrol® 220) was subsequently released at two locations at the sand surface. Visible light transmission was used to quantitatively determine water saturations prior to LNAPL release and to observe LNAPL flow paths. Numerical simulations were performed using the Subsurface Transport Over Multiple Phases (STOMP) simulator, employing two nonhysteretic relative permeability–saturation–pressure (
k–
S–
P) models. LNAPL movement strongly depended on the water saturation in the fine-grained sand layer above the textural interface. In general, reasonable agreement was found between observed and predicted water saturations near the textural interface and LNAPL flow paths. Discrepancies between predictions based on the van Genuchten/Mualem (VGM) and Brooks–Corey/Burdine (BCB)
k–
S–
P models existed in the migration speed of the simulated LNAPL plume and the LNAPL flow patterns at high water saturation above the textural interface. In both instances, predictions based on the BCB model agreed better with experimental observations than predictions based on the VGM model. The results confirm the critical role water saturation plays in determining LNAPL movement in heterogeneous vadose zone environments and that accurate prediction of LNAPL flow paths depends on the careful selection of an appropriate
k–
S–
P model.</description><identifier>ISSN: 0309-1708</identifier><identifier>EISSN: 1872-9657</identifier><identifier>DOI: 10.1016/S0309-1708(97)00043-2</identifier><identifier>CODEN: AWREDI</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>BENCH-SCALE EXPERIMENTS ; capillary barrier ; COMPUTERIZED SIMULATION ; constitutive relations ; Earth sciences ; Earth, ocean, space ; Engineering and environment geology. Geothermics ; ENVIRONMENTAL SCIENCES ; Exact sciences and technology ; Hydrogeology ; Hydrology. Hydrogeology ; LNAPL ; multifluid flow ; MULTIPHASE FLOW ; numerical simulation ; Pollution, environment geology ; POROUS MATERIALS</subject><ispartof>Advances in Water Resources, 22(2):169-183, 1998-10, Vol.22 (2), p.169-183</ispartof><rights>1998 Elsevier Science Ltd</rights><rights>1999 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a449t-a0b6cc604df0c752fb06e21566d1e77cb7820d52d563fd28f01bd607f55662973</citedby><cites>FETCH-LOGICAL-a449t-a0b6cc604df0c752fb06e21566d1e77cb7820d52d563fd28f01bd607f55662973</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0309170897000432$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,881,3537,27901,27902,65306</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=1598545$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/15001684$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Schroth, M.H.</creatorcontrib><creatorcontrib>Istok, J.D.</creatorcontrib><creatorcontrib>Selker, J.S.</creatorcontrib><creatorcontrib>Oostrom, M.</creatorcontrib><creatorcontrib>White, M.D.</creatorcontrib><creatorcontrib>Pacific Northwest National Lab. (PNNL), Richland, WA (United States)</creatorcontrib><title>Multifluid flow in bedded porous media: laboratory experiments and numerical simulations</title><title>Advances in Water Resources, 22(2):169-183</title><description>Understanding light nonaqueous-phase liquid (LNAPL) movement in heterogeneous vadose environments is important for effective remediation design. We investigated LNAPL movement near a sloping fine- over coarse-grained textural interface, forming a capillary barrier. LNAPL flow experiments were performed in a glass chamber (50
cm×60
cm×1.0
cm) using two silica sands (12/20 and 30/40 sieve sizes). Variable water saturations near the textural interface were generated by applying water uniformly to the sand surface at various flow rates. A model LNAPL (Soltrol® 220) was subsequently released at two locations at the sand surface. Visible light transmission was used to quantitatively determine water saturations prior to LNAPL release and to observe LNAPL flow paths. Numerical simulations were performed using the Subsurface Transport Over Multiple Phases (STOMP) simulator, employing two nonhysteretic relative permeability–saturation–pressure (
k–
S–
P) models. LNAPL movement strongly depended on the water saturation in the fine-grained sand layer above the textural interface. In general, reasonable agreement was found between observed and predicted water saturations near the textural interface and LNAPL flow paths. Discrepancies between predictions based on the van Genuchten/Mualem (VGM) and Brooks–Corey/Burdine (BCB)
k–
S–
P models existed in the migration speed of the simulated LNAPL plume and the LNAPL flow patterns at high water saturation above the textural interface. In both instances, predictions based on the BCB model agreed better with experimental observations than predictions based on the VGM model. The results confirm the critical role water saturation plays in determining LNAPL movement in heterogeneous vadose zone environments and that accurate prediction of LNAPL flow paths depends on the careful selection of an appropriate
k–
S–
P model.</description><subject>BENCH-SCALE EXPERIMENTS</subject><subject>capillary barrier</subject><subject>COMPUTERIZED SIMULATION</subject><subject>constitutive relations</subject><subject>Earth sciences</subject><subject>Earth, ocean, space</subject><subject>Engineering and environment geology. Geothermics</subject><subject>ENVIRONMENTAL SCIENCES</subject><subject>Exact sciences and technology</subject><subject>Hydrogeology</subject><subject>Hydrology. Hydrogeology</subject><subject>LNAPL</subject><subject>multifluid flow</subject><subject>MULTIPHASE FLOW</subject><subject>numerical simulation</subject><subject>Pollution, environment geology</subject><subject>POROUS MATERIALS</subject><issn>0309-1708</issn><issn>1872-9657</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><recordid>eNqFkU1rFTEUhoMoeK3-BCGgSF2MPclMkhk3IsUvaHGhgruQSU4wMpNck4y2_97c3qLLrkLgOefwPi8hTxm8YsDk2RfoYeqYgvF0Ui8BYOg7fo_s2Kh4N0mh7pPdP-QheVTKzwaNg-I78v1yW2rwyxYc9Uv6Q0OkMzqHju5TTluhK7pgXtPFzCmbmvI1xas95rBirIWa6Gjc1va3ZqElrNtiakixPCYPvFkKPrl9T8i39---nn_sLj5_-HT-9qIzwzDVzsAsrZUwOA9WCe5nkMiZkNIxVMrOauTgBHdC9t7x0QObnQTlRUP4pPoT8uy4N5UadLGhov1hU4xoq2YCmqBxaNSLI7XP6deGpeo1FIvLYiK2kJopxkBO7G6wl7If-rGB4gjanErJ6PW-OTH5WjPQh1r0TS364FxPSt_Uonmbe357wJSmzGcTbSj_h8U0ikE07M0Rw-bud8B8iIbRtjLyIZlL4Y5DfwEjLKD7</recordid><startdate>19981022</startdate><enddate>19981022</enddate><creator>Schroth, M.H.</creator><creator>Istok, J.D.</creator><creator>Selker, J.S.</creator><creator>Oostrom, M.</creator><creator>White, M.D.</creator><general>Elsevier Ltd</general><general>Elsevier Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QH</scope><scope>7UA</scope><scope>C1K</scope><scope>OTOTI</scope></search><sort><creationdate>19981022</creationdate><title>Multifluid flow in bedded porous media: laboratory experiments and numerical simulations</title><author>Schroth, M.H. ; Istok, J.D. ; Selker, J.S. ; Oostrom, M. ; White, M.D.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a449t-a0b6cc604df0c752fb06e21566d1e77cb7820d52d563fd28f01bd607f55662973</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>BENCH-SCALE EXPERIMENTS</topic><topic>capillary barrier</topic><topic>COMPUTERIZED SIMULATION</topic><topic>constitutive relations</topic><topic>Earth sciences</topic><topic>Earth, ocean, space</topic><topic>Engineering and environment geology. Geothermics</topic><topic>ENVIRONMENTAL SCIENCES</topic><topic>Exact sciences and technology</topic><topic>Hydrogeology</topic><topic>Hydrology. Hydrogeology</topic><topic>LNAPL</topic><topic>multifluid flow</topic><topic>MULTIPHASE FLOW</topic><topic>numerical simulation</topic><topic>Pollution, environment geology</topic><topic>POROUS MATERIALS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schroth, M.H.</creatorcontrib><creatorcontrib>Istok, J.D.</creatorcontrib><creatorcontrib>Selker, J.S.</creatorcontrib><creatorcontrib>Oostrom, M.</creatorcontrib><creatorcontrib>White, M.D.</creatorcontrib><creatorcontrib>Pacific Northwest National Lab. (PNNL), Richland, WA (United States)</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Aqualine</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><collection>OSTI.GOV</collection><jtitle>Advances in Water Resources, 22(2):169-183</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schroth, M.H.</au><au>Istok, J.D.</au><au>Selker, J.S.</au><au>Oostrom, M.</au><au>White, M.D.</au><aucorp>Pacific Northwest National Lab. (PNNL), Richland, WA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Multifluid flow in bedded porous media: laboratory experiments and numerical simulations</atitle><jtitle>Advances in Water Resources, 22(2):169-183</jtitle><date>1998-10-22</date><risdate>1998</risdate><volume>22</volume><issue>2</issue><spage>169</spage><epage>183</epage><pages>169-183</pages><issn>0309-1708</issn><eissn>1872-9657</eissn><coden>AWREDI</coden><abstract>Understanding light nonaqueous-phase liquid (LNAPL) movement in heterogeneous vadose environments is important for effective remediation design. We investigated LNAPL movement near a sloping fine- over coarse-grained textural interface, forming a capillary barrier. LNAPL flow experiments were performed in a glass chamber (50
cm×60
cm×1.0
cm) using two silica sands (12/20 and 30/40 sieve sizes). Variable water saturations near the textural interface were generated by applying water uniformly to the sand surface at various flow rates. A model LNAPL (Soltrol® 220) was subsequently released at two locations at the sand surface. Visible light transmission was used to quantitatively determine water saturations prior to LNAPL release and to observe LNAPL flow paths. Numerical simulations were performed using the Subsurface Transport Over Multiple Phases (STOMP) simulator, employing two nonhysteretic relative permeability–saturation–pressure (
k–
S–
P) models. LNAPL movement strongly depended on the water saturation in the fine-grained sand layer above the textural interface. In general, reasonable agreement was found between observed and predicted water saturations near the textural interface and LNAPL flow paths. Discrepancies between predictions based on the van Genuchten/Mualem (VGM) and Brooks–Corey/Burdine (BCB)
k–
S–
P models existed in the migration speed of the simulated LNAPL plume and the LNAPL flow patterns at high water saturation above the textural interface. In both instances, predictions based on the BCB model agreed better with experimental observations than predictions based on the VGM model. The results confirm the critical role water saturation plays in determining LNAPL movement in heterogeneous vadose zone environments and that accurate prediction of LNAPL flow paths depends on the careful selection of an appropriate
k–
S–
P model.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/S0309-1708(97)00043-2</doi><tpages>15</tpages></addata></record> |
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language | eng |
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source | Elsevier ScienceDirect Journals |
subjects | BENCH-SCALE EXPERIMENTS capillary barrier COMPUTERIZED SIMULATION constitutive relations Earth sciences Earth, ocean, space Engineering and environment geology. Geothermics ENVIRONMENTAL SCIENCES Exact sciences and technology Hydrogeology Hydrology. Hydrogeology LNAPL multifluid flow MULTIPHASE FLOW numerical simulation Pollution, environment geology POROUS MATERIALS |
title | Multifluid flow in bedded porous media: laboratory experiments and numerical simulations |
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