Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments
Experimental observations of the dissolution of calcium sulfate by flowing water have been used to investigate the assumptions underlying pore-scale models of reactive transport. Microfluidic experiments were designed to observe changes in size and shape as cylindrical disks (radius 10 mm) of gypsum...
Gespeichert in:
Veröffentlicht in: | Chemical geology 2020-05, Vol.540 (C), p.119459, Article 119459 |
---|---|
Hauptverfasser: | , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | |
---|---|
container_issue | C |
container_start_page | 119459 |
container_title | Chemical geology |
container_volume | 540 |
creator | Dutka, Filip Starchenko, Vitaliy Osselin, Florian Magni, Silvana Szymczak, Piotr Ladd, Anthony J.C. |
description | Experimental observations of the dissolution of calcium sulfate by flowing water have been used to investigate the assumptions underlying pore-scale models of reactive transport. Microfluidic experiments were designed to observe changes in size and shape as cylindrical disks (radius 10 mm) of gypsum dissolved for periods of up to 40 days. The dissolution flux over the whole surface of the sample can be determined by observing the motion of the interface. However, in order to extract surface reaction rates, numerical simulations are required to account for diffusional hindrance across the concentration boundary layer; the geometry is too complex for analytic solutions.
We have found that a first-principles simulation of pore-scale flow and transport, with a single value of the surface reaction rate, was able to reproduce the time sequence of sample shapes without any fitting parameters. The value of the rate constant is close to recent experimental measurements but much smaller than some earlier values. The shape evolution is a more stringent test of the validity of the method than average measurements such as effluent concentration, because it requires the correct flux at each point on the sample surface.
Shapes of a dissolving gypsum chip: comparison of simulations with a microfluidic experiment. The images are photographs of the experiment at different times. The initially circular sample (white line) dissolves in the flow of water (left to right) and takes up an asymmetric shape front to back (white region). The colored lines indicate shapes from numerical simulations at the same times - there are no fitting parameters in these comparisons. The blue lines indicate results using the infinite-dilution diffusion coefficient; the red lines include corrections due to the finite concentration of the ions. [Display omitted]
•Developed a microfluidic experiment to probe local dissolution rates•Simulations are needed to account for ion diffusion across the boundary layer.•Simulated shapes matched experimental observations with a single rate constant.•Rate constant is close to accepted value for gypsum dissolution.•Inclusion of finite concentration effects improves agreement with experiment. |
doi_str_mv | 10.1016/j.chemgeo.2019.119459 |
format | Article |
fullrecord | <record><control><sourceid>hal_osti_</sourceid><recordid>TN_cdi_osti_scitechconnect_1606995</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0009254119305881</els_id><sourcerecordid>oai_HAL_insu_02512853v1</sourcerecordid><originalsourceid>FETCH-LOGICAL-a441t-da7c0e0563cb5ae4c04ea88564201eb4fbd77598934d1af11660b1529452652e3</originalsourceid><addsrcrecordid>eNqFkUGL2zAQhUVpoeluf0LB9FhwqrElxe6lLKHdLQR62Z6FIo3jCbZkJCft_vvK9bLXnoaB7828x2PsA_AtcFCfz1vb43jCsK04tFuAVsj2FdtAs6tK1dTqNdtwztuykgLesncpnfMKtZQbNj7SiKXDCb1DPxepNxOmInSFKRylFIYr-VMxksdohuIUDfkvxT6Mk4mUgv-HJhovg5lpWX_T3GfcxtANF3JkC_wzYcxf_Jxu2ZvODAnfP88b9uv7t8f9Q3n4ef9jf3cojRAwl87sLEcuVW2P0qCwXKBpGqlEDohH0R3dbifbpq2FA9MBKMWPIKucu1KywvqGfVzvhjSTTpZmtL0N3qOdNSiu2lZm6NMK9WbQU3Zo4pMOhvTD3UGTTxfNKwlVI-srZFiucA6WUsTuRQFcLy3os35uQS8t6LWFrPu66jDHvRLGxQ16i47iYsYF-s-Fv4Dtk94</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments</title><source>Elsevier ScienceDirect Journals</source><creator>Dutka, Filip ; Starchenko, Vitaliy ; Osselin, Florian ; Magni, Silvana ; Szymczak, Piotr ; Ladd, Anthony J.C.</creator><creatorcontrib>Dutka, Filip ; Starchenko, Vitaliy ; Osselin, Florian ; Magni, Silvana ; Szymczak, Piotr ; Ladd, Anthony J.C. ; Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><description>Experimental observations of the dissolution of calcium sulfate by flowing water have been used to investigate the assumptions underlying pore-scale models of reactive transport. Microfluidic experiments were designed to observe changes in size and shape as cylindrical disks (radius 10 mm) of gypsum dissolved for periods of up to 40 days. The dissolution flux over the whole surface of the sample can be determined by observing the motion of the interface. However, in order to extract surface reaction rates, numerical simulations are required to account for diffusional hindrance across the concentration boundary layer; the geometry is too complex for analytic solutions.
We have found that a first-principles simulation of pore-scale flow and transport, with a single value of the surface reaction rate, was able to reproduce the time sequence of sample shapes without any fitting parameters. The value of the rate constant is close to recent experimental measurements but much smaller than some earlier values. The shape evolution is a more stringent test of the validity of the method than average measurements such as effluent concentration, because it requires the correct flux at each point on the sample surface.
Shapes of a dissolving gypsum chip: comparison of simulations with a microfluidic experiment. The images are photographs of the experiment at different times. The initially circular sample (white line) dissolves in the flow of water (left to right) and takes up an asymmetric shape front to back (white region). The colored lines indicate shapes from numerical simulations at the same times - there are no fitting parameters in these comparisons. The blue lines indicate results using the infinite-dilution diffusion coefficient; the red lines include corrections due to the finite concentration of the ions. [Display omitted]
•Developed a microfluidic experiment to probe local dissolution rates•Simulations are needed to account for ion diffusion across the boundary layer.•Simulated shapes matched experimental observations with a single rate constant.•Rate constant is close to accepted value for gypsum dissolution.•Inclusion of finite concentration effects improves agreement with experiment.</description><identifier>ISSN: 0009-2541</identifier><identifier>EISSN: 1872-6836</identifier><identifier>DOI: 10.1016/j.chemgeo.2019.119459</identifier><language>eng</language><publisher>United States: Elsevier B.V</publisher><subject>Dissolution rate ; GEOSCIENCES ; Gypsum dissolution ; INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY ; Pore scale modeling ; Reactive surface area ; Sciences of the Universe ; Simulation and experiment</subject><ispartof>Chemical geology, 2020-05, Vol.540 (C), p.119459, Article 119459</ispartof><rights>2020 The Authors</rights><rights>Attribution - NonCommercial</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a441t-da7c0e0563cb5ae4c04ea88564201eb4fbd77598934d1af11660b1529452652e3</citedby><cites>FETCH-LOGICAL-a441t-da7c0e0563cb5ae4c04ea88564201eb4fbd77598934d1af11660b1529452652e3</cites><orcidid>0000-0003-2313-7379 ; 0000-0002-0271-0650 ; 0000-0003-1991-7153 ; 0000000319917153 ; 0000000323137379 ; 0000000202710650</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0009254119305881$$EHTML$$P50$$Gelsevier$$Hfree_for_read</linktohtml><link.rule.ids>230,314,776,780,881,3537,27901,27902,65306</link.rule.ids><backlink>$$Uhttps://insu.hal.science/insu-02512853$$DView record in HAL$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/servlets/purl/1606995$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Dutka, Filip</creatorcontrib><creatorcontrib>Starchenko, Vitaliy</creatorcontrib><creatorcontrib>Osselin, Florian</creatorcontrib><creatorcontrib>Magni, Silvana</creatorcontrib><creatorcontrib>Szymczak, Piotr</creatorcontrib><creatorcontrib>Ladd, Anthony J.C.</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><title>Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments</title><title>Chemical geology</title><description>Experimental observations of the dissolution of calcium sulfate by flowing water have been used to investigate the assumptions underlying pore-scale models of reactive transport. Microfluidic experiments were designed to observe changes in size and shape as cylindrical disks (radius 10 mm) of gypsum dissolved for periods of up to 40 days. The dissolution flux over the whole surface of the sample can be determined by observing the motion of the interface. However, in order to extract surface reaction rates, numerical simulations are required to account for diffusional hindrance across the concentration boundary layer; the geometry is too complex for analytic solutions.
We have found that a first-principles simulation of pore-scale flow and transport, with a single value of the surface reaction rate, was able to reproduce the time sequence of sample shapes without any fitting parameters. The value of the rate constant is close to recent experimental measurements but much smaller than some earlier values. The shape evolution is a more stringent test of the validity of the method than average measurements such as effluent concentration, because it requires the correct flux at each point on the sample surface.
Shapes of a dissolving gypsum chip: comparison of simulations with a microfluidic experiment. The images are photographs of the experiment at different times. The initially circular sample (white line) dissolves in the flow of water (left to right) and takes up an asymmetric shape front to back (white region). The colored lines indicate shapes from numerical simulations at the same times - there are no fitting parameters in these comparisons. The blue lines indicate results using the infinite-dilution diffusion coefficient; the red lines include corrections due to the finite concentration of the ions. [Display omitted]
•Developed a microfluidic experiment to probe local dissolution rates•Simulations are needed to account for ion diffusion across the boundary layer.•Simulated shapes matched experimental observations with a single rate constant.•Rate constant is close to accepted value for gypsum dissolution.•Inclusion of finite concentration effects improves agreement with experiment.</description><subject>Dissolution rate</subject><subject>GEOSCIENCES</subject><subject>Gypsum dissolution</subject><subject>INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY</subject><subject>Pore scale modeling</subject><subject>Reactive surface area</subject><subject>Sciences of the Universe</subject><subject>Simulation and experiment</subject><issn>0009-2541</issn><issn>1872-6836</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNqFkUGL2zAQhUVpoeluf0LB9FhwqrElxe6lLKHdLQR62Z6FIo3jCbZkJCft_vvK9bLXnoaB7828x2PsA_AtcFCfz1vb43jCsK04tFuAVsj2FdtAs6tK1dTqNdtwztuykgLesncpnfMKtZQbNj7SiKXDCb1DPxepNxOmInSFKRylFIYr-VMxksdohuIUDfkvxT6Mk4mUgv-HJhovg5lpWX_T3GfcxtANF3JkC_wzYcxf_Jxu2ZvODAnfP88b9uv7t8f9Q3n4ef9jf3cojRAwl87sLEcuVW2P0qCwXKBpGqlEDohH0R3dbifbpq2FA9MBKMWPIKucu1KywvqGfVzvhjSTTpZmtL0N3qOdNSiu2lZm6NMK9WbQU3Zo4pMOhvTD3UGTTxfNKwlVI-srZFiucA6WUsTuRQFcLy3os35uQS8t6LWFrPu66jDHvRLGxQ16i47iYsYF-s-Fv4Dtk94</recordid><startdate>20200505</startdate><enddate>20200505</enddate><creator>Dutka, Filip</creator><creator>Starchenko, Vitaliy</creator><creator>Osselin, Florian</creator><creator>Magni, Silvana</creator><creator>Szymczak, Piotr</creator><creator>Ladd, Anthony J.C.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>6I.</scope><scope>AAFTH</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><scope>VOOES</scope><scope>OIOZB</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-2313-7379</orcidid><orcidid>https://orcid.org/0000-0002-0271-0650</orcidid><orcidid>https://orcid.org/0000-0003-1991-7153</orcidid><orcidid>https://orcid.org/0000000319917153</orcidid><orcidid>https://orcid.org/0000000323137379</orcidid><orcidid>https://orcid.org/0000000202710650</orcidid></search><sort><creationdate>20200505</creationdate><title>Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments</title><author>Dutka, Filip ; Starchenko, Vitaliy ; Osselin, Florian ; Magni, Silvana ; Szymczak, Piotr ; Ladd, Anthony J.C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a441t-da7c0e0563cb5ae4c04ea88564201eb4fbd77598934d1af11660b1529452652e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Dissolution rate</topic><topic>GEOSCIENCES</topic><topic>Gypsum dissolution</topic><topic>INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY</topic><topic>Pore scale modeling</topic><topic>Reactive surface area</topic><topic>Sciences of the Universe</topic><topic>Simulation and experiment</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dutka, Filip</creatorcontrib><creatorcontrib>Starchenko, Vitaliy</creatorcontrib><creatorcontrib>Osselin, Florian</creatorcontrib><creatorcontrib>Magni, Silvana</creatorcontrib><creatorcontrib>Szymczak, Piotr</creatorcontrib><creatorcontrib>Ladd, Anthony J.C.</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><collection>ScienceDirect Open Access Titles</collection><collection>Elsevier:ScienceDirect:Open Access</collection><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Chemical geology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dutka, Filip</au><au>Starchenko, Vitaliy</au><au>Osselin, Florian</au><au>Magni, Silvana</au><au>Szymczak, Piotr</au><au>Ladd, Anthony J.C.</au><aucorp>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments</atitle><jtitle>Chemical geology</jtitle><date>2020-05-05</date><risdate>2020</risdate><volume>540</volume><issue>C</issue><spage>119459</spage><pages>119459-</pages><artnum>119459</artnum><issn>0009-2541</issn><eissn>1872-6836</eissn><abstract>Experimental observations of the dissolution of calcium sulfate by flowing water have been used to investigate the assumptions underlying pore-scale models of reactive transport. Microfluidic experiments were designed to observe changes in size and shape as cylindrical disks (radius 10 mm) of gypsum dissolved for periods of up to 40 days. The dissolution flux over the whole surface of the sample can be determined by observing the motion of the interface. However, in order to extract surface reaction rates, numerical simulations are required to account for diffusional hindrance across the concentration boundary layer; the geometry is too complex for analytic solutions.
We have found that a first-principles simulation of pore-scale flow and transport, with a single value of the surface reaction rate, was able to reproduce the time sequence of sample shapes without any fitting parameters. The value of the rate constant is close to recent experimental measurements but much smaller than some earlier values. The shape evolution is a more stringent test of the validity of the method than average measurements such as effluent concentration, because it requires the correct flux at each point on the sample surface.
Shapes of a dissolving gypsum chip: comparison of simulations with a microfluidic experiment. The images are photographs of the experiment at different times. The initially circular sample (white line) dissolves in the flow of water (left to right) and takes up an asymmetric shape front to back (white region). The colored lines indicate shapes from numerical simulations at the same times - there are no fitting parameters in these comparisons. The blue lines indicate results using the infinite-dilution diffusion coefficient; the red lines include corrections due to the finite concentration of the ions. [Display omitted]
•Developed a microfluidic experiment to probe local dissolution rates•Simulations are needed to account for ion diffusion across the boundary layer.•Simulated shapes matched experimental observations with a single rate constant.•Rate constant is close to accepted value for gypsum dissolution.•Inclusion of finite concentration effects improves agreement with experiment.</abstract><cop>United States</cop><pub>Elsevier B.V</pub><doi>10.1016/j.chemgeo.2019.119459</doi><orcidid>https://orcid.org/0000-0003-2313-7379</orcidid><orcidid>https://orcid.org/0000-0002-0271-0650</orcidid><orcidid>https://orcid.org/0000-0003-1991-7153</orcidid><orcidid>https://orcid.org/0000000319917153</orcidid><orcidid>https://orcid.org/0000000323137379</orcidid><orcidid>https://orcid.org/0000000202710650</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0009-2541 |
ispartof | Chemical geology, 2020-05, Vol.540 (C), p.119459, Article 119459 |
issn | 0009-2541 1872-6836 |
language | eng |
recordid | cdi_osti_scitechconnect_1606995 |
source | Elsevier ScienceDirect Journals |
subjects | Dissolution rate GEOSCIENCES Gypsum dissolution INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY Pore scale modeling Reactive surface area Sciences of the Universe Simulation and experiment |
title | Time-dependent shapes of a dissolving mineral grain: Comparisons of simulations with microfluidic experiments |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-30T23%3A22%3A50IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-hal_osti_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Time-dependent%20shapes%20of%20a%20dissolving%20mineral%20grain:%20Comparisons%20of%20simulations%20with%20microfluidic%20experiments&rft.jtitle=Chemical%20geology&rft.au=Dutka,%20Filip&rft.aucorp=Oak%20Ridge%20National%20Lab.%20(ORNL),%20Oak%20Ridge,%20TN%20(United%20States)&rft.date=2020-05-05&rft.volume=540&rft.issue=C&rft.spage=119459&rft.pages=119459-&rft.artnum=119459&rft.issn=0009-2541&rft.eissn=1872-6836&rft_id=info:doi/10.1016/j.chemgeo.2019.119459&rft_dat=%3Chal_osti_%3Eoai_HAL_insu_02512853v1%3C/hal_osti_%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rft_els_id=S0009254119305881&rfr_iscdi=true |