Time–connectivity superposition and the gel/glass duality of weak colloidal gels
Colloidal gels result from the aggregation of Brownian particles suspended in a solvent. Gelation is induced by attractive interactions between individual particles that drive the formation of clusters, which in turn aggregate to form a space-spanning structure. We study this process in aluminosilic...
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creator | Keshavarz, Bavand Rodrigues, Donatien Gomes Champenois, Jean-Baptiste Frith, Matthew G. Ilavsky, Jan Geri, Michela Divoux, Thibaut McKinley, Gareth H. Poulesquen, Arnaud |
description | Colloidal gels result from the aggregation of Brownian particles suspended in a solvent. Gelation is induced by attractive interactions between individual particles that drive the formation of clusters, which in turn aggregate to form a space-spanning structure. We study this process in aluminosilicate colloidal gels through time-resolved structural and mechanical spectroscopy. Using the time–connectivity superposition principle a series of rapidly acquired linear viscoelastic spectra, measured throughout the gelation process by applying an exponential chirp protocol, are rescaled onto a universal master curve that spans over eight orders of magnitude in reduced frequency. This analysis reveals that the underlying relaxation time spectrum of the colloidal gel is symmetric in time with power-law tails characterized by a single exponent that is set at the gel point. The microstructural mechanical network has a dual character; at short length scales and fast times it appears glassy, whereas at longer times and larger scales it is gel-like. These results can be captured by a simple three-parameter constitutive model and demonstrate that the microstructure of a mature colloidal gel bears the residual skeleton of the original sample-spanning network that is created at the gel point. Our conclusions are confirmed by applying the same technique to another well-known colloidal gel system composed of attractive silica nanoparticles. The results illustrate the power of the time–connectivity superposition principle for this class of soft glassy materials and provide a compact description for the dichotomous viscoelastic nature of weak colloidal gels. |
doi_str_mv | 10.1073/pnas.2022339118 |
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(ANL), Argonne, IL (United States)</creatorcontrib><description>Colloidal gels result from the aggregation of Brownian particles suspended in a solvent. Gelation is induced by attractive interactions between individual particles that drive the formation of clusters, which in turn aggregate to form a space-spanning structure. We study this process in aluminosilicate colloidal gels through time-resolved structural and mechanical spectroscopy. Using the time–connectivity superposition principle a series of rapidly acquired linear viscoelastic spectra, measured throughout the gelation process by applying an exponential chirp protocol, are rescaled onto a universal master curve that spans over eight orders of magnitude in reduced frequency. This analysis reveals that the underlying relaxation time spectrum of the colloidal gel is symmetric in time with power-law tails characterized by a single exponent that is set at the gel point. The microstructural mechanical network has a dual character; at short length scales and fast times it appears glassy, whereas at longer times and larger scales it is gel-like. These results can be captured by a simple three-parameter constitutive model and demonstrate that the microstructure of a mature colloidal gel bears the residual skeleton of the original sample-spanning network that is created at the gel point. Our conclusions are confirmed by applying the same technique to another well-known colloidal gel system composed of attractive silica nanoparticles. The results illustrate the power of the time–connectivity superposition principle for this class of soft glassy materials and provide a compact description for the dichotomous viscoelastic nature of weak colloidal gels.</description><identifier>ISSN: 0027-8424</identifier><identifier>EISSN: 1091-6490</identifier><identifier>DOI: 10.1073/pnas.2022339118</identifier><identifier>PMID: 33837153</identifier><language>eng</language><publisher>United States: National Academy of Sciences</publisher><subject>aluminosilicate ; Aluminosilicates ; Aluminum silicates ; Brownian motion ; Colloiding ; Condensed Matter ; Connectivity ; Constitutive models ; Frequency analysis ; Gelation ; Gels ; gels and glasses ; MATERIALS SCIENCE ; Microstructure ; Nanoparticles ; Physical Sciences ; Physics ; Relaxation time ; relaxation time spectrum ; Silica ; Silicon dioxide ; Soft Condensed Matter ; Spectroscopy ; Spectrum analysis ; Superposition (mathematics) ; time-connectivity superposition ; Viscoelasticity ; weak colloidal gels</subject><ispartof>Proceedings of the National Academy of Sciences - PNAS, 2021-04, Vol.118 (15), p.1-9</ispartof><rights>Copyright National Academy of Sciences Apr 13, 2021</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><rights>2021</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c504t-6ef119202437bedc4d4ba9dff7d6f2273baad1abbdfdf6f6c51964aee05e5ccc3</citedby><cites>FETCH-LOGICAL-c504t-6ef119202437bedc4d4ba9dff7d6f2273baad1abbdfdf6f6c51964aee05e5ccc3</cites><orcidid>0000-0002-6393-5378 ; 0000-0002-9169-7434 ; 0000-0002-6777-5084 ; 0000-0003-1982-8900 ; 0000-0001-8323-2779 ; 0000-0003-1725-3912 ; 0000-0002-1988-8500 ; 0000-0002-5587-7892 ; 0000000291697434 ; 0000000183232779 ; 0000000317253912 ; 0000000263935378 ; 0000000319828900 ; 0000000267775084 ; 0000000219888500</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/27040096$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/27040096$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>230,314,723,776,780,799,881,27903,27904,53769,53771,57995,58228</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/33837153$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://cea.hal.science/cea-03327873$$DView record in HAL$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/servlets/purl/1798453$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Keshavarz, Bavand</creatorcontrib><creatorcontrib>Rodrigues, Donatien Gomes</creatorcontrib><creatorcontrib>Champenois, Jean-Baptiste</creatorcontrib><creatorcontrib>Frith, Matthew G.</creatorcontrib><creatorcontrib>Ilavsky, Jan</creatorcontrib><creatorcontrib>Geri, Michela</creatorcontrib><creatorcontrib>Divoux, Thibaut</creatorcontrib><creatorcontrib>McKinley, Gareth H.</creatorcontrib><creatorcontrib>Poulesquen, Arnaud</creatorcontrib><creatorcontrib>Argonne National Lab. (ANL), Argonne, IL (United States)</creatorcontrib><title>Time–connectivity superposition and the gel/glass duality of weak colloidal gels</title><title>Proceedings of the National Academy of Sciences - PNAS</title><addtitle>Proc Natl Acad Sci U S A</addtitle><description>Colloidal gels result from the aggregation of Brownian particles suspended in a solvent. Gelation is induced by attractive interactions between individual particles that drive the formation of clusters, which in turn aggregate to form a space-spanning structure. We study this process in aluminosilicate colloidal gels through time-resolved structural and mechanical spectroscopy. Using the time–connectivity superposition principle a series of rapidly acquired linear viscoelastic spectra, measured throughout the gelation process by applying an exponential chirp protocol, are rescaled onto a universal master curve that spans over eight orders of magnitude in reduced frequency. This analysis reveals that the underlying relaxation time spectrum of the colloidal gel is symmetric in time with power-law tails characterized by a single exponent that is set at the gel point. The microstructural mechanical network has a dual character; at short length scales and fast times it appears glassy, whereas at longer times and larger scales it is gel-like. These results can be captured by a simple three-parameter constitutive model and demonstrate that the microstructure of a mature colloidal gel bears the residual skeleton of the original sample-spanning network that is created at the gel point. Our conclusions are confirmed by applying the same technique to another well-known colloidal gel system composed of attractive silica nanoparticles. The results illustrate the power of the time–connectivity superposition principle for this class of soft glassy materials and provide a compact description for the dichotomous viscoelastic nature of weak colloidal gels.</description><subject>aluminosilicate</subject><subject>Aluminosilicates</subject><subject>Aluminum silicates</subject><subject>Brownian motion</subject><subject>Colloiding</subject><subject>Condensed Matter</subject><subject>Connectivity</subject><subject>Constitutive models</subject><subject>Frequency analysis</subject><subject>Gelation</subject><subject>Gels</subject><subject>gels and glasses</subject><subject>MATERIALS SCIENCE</subject><subject>Microstructure</subject><subject>Nanoparticles</subject><subject>Physical Sciences</subject><subject>Physics</subject><subject>Relaxation time</subject><subject>relaxation time spectrum</subject><subject>Silica</subject><subject>Silicon dioxide</subject><subject>Soft Condensed Matter</subject><subject>Spectroscopy</subject><subject>Spectrum analysis</subject><subject>Superposition (mathematics)</subject><subject>time-connectivity superposition</subject><subject>Viscoelasticity</subject><subject>weak colloidal gels</subject><issn>0027-8424</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNpd0k2LEzEYB_AgiltXz56UQS96mG1eJ5PLwrKoKxQEWc8hk5c2NZ3USaayN7-D39BPYoapVfeUQ3758_DPA8BzBC8Q5GS571W6wBBjQgRC7QOwQFCguqECPgQLCDGvW4rpGXiS0hZCKFgLH4MzQlrCESML8PnW7-yvHz917Hursz_4fFelcW-HfUw--9hXqjdV3thqbcNyHVRKlRlVmFx01XervlY6hhC9UWEy6Sl45FRI9tnxPAdf3r-7vb6pV58-fLy-WtWaQZrrxjqERJmdEt5Zo6mhnRLGOW4ahzEnnVIGqa4zzrjGNZoh0VBlLWSWaa3JObicc_djtysBts-DCnI_-J0a7mRUXv5_0_uNXMeDbCGjEDYl4NUcEFP2Mmmfrd4ci5CIi5YyUtDbGW3uZd9craS2SkJCMG85OaBi3xwnGuK30aYsdz5pG4LqbRyTxAwhTCnlbaGv79FtHIe-9DUpggVkbFLLWekhpjRYd5oAQTktgJwWQP5dgPLi5b-lnPyfHy_gxQy2KcfhdI85LJ2IhvwGziq4Jw</recordid><startdate>20210413</startdate><enddate>20210413</enddate><creator>Keshavarz, Bavand</creator><creator>Rodrigues, Donatien Gomes</creator><creator>Champenois, Jean-Baptiste</creator><creator>Frith, Matthew G.</creator><creator>Ilavsky, Jan</creator><creator>Geri, Michela</creator><creator>Divoux, Thibaut</creator><creator>McKinley, Gareth H.</creator><creator>Poulesquen, Arnaud</creator><general>National Academy of Sciences</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QG</scope><scope>7QL</scope><scope>7QP</scope><scope>7QR</scope><scope>7SN</scope><scope>7SS</scope><scope>7T5</scope><scope>7TK</scope><scope>7TM</scope><scope>7TO</scope><scope>7U9</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H94</scope><scope>M7N</scope><scope>P64</scope><scope>RC3</scope><scope>7X8</scope><scope>1XC</scope><scope>OIOZB</scope><scope>OTOTI</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0002-6393-5378</orcidid><orcidid>https://orcid.org/0000-0002-9169-7434</orcidid><orcidid>https://orcid.org/0000-0002-6777-5084</orcidid><orcidid>https://orcid.org/0000-0003-1982-8900</orcidid><orcidid>https://orcid.org/0000-0001-8323-2779</orcidid><orcidid>https://orcid.org/0000-0003-1725-3912</orcidid><orcidid>https://orcid.org/0000-0002-1988-8500</orcidid><orcidid>https://orcid.org/0000-0002-5587-7892</orcidid><orcidid>https://orcid.org/0000000291697434</orcidid><orcidid>https://orcid.org/0000000183232779</orcidid><orcidid>https://orcid.org/0000000317253912</orcidid><orcidid>https://orcid.org/0000000263935378</orcidid><orcidid>https://orcid.org/0000000319828900</orcidid><orcidid>https://orcid.org/0000000267775084</orcidid><orcidid>https://orcid.org/0000000219888500</orcidid></search><sort><creationdate>20210413</creationdate><title>Time–connectivity superposition and the gel/glass duality of weak colloidal gels</title><author>Keshavarz, Bavand ; Rodrigues, Donatien Gomes ; Champenois, Jean-Baptiste ; Frith, Matthew G. ; Ilavsky, Jan ; Geri, Michela ; Divoux, Thibaut ; McKinley, Gareth H. ; Poulesquen, Arnaud</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c504t-6ef119202437bedc4d4ba9dff7d6f2273baad1abbdfdf6f6c51964aee05e5ccc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>aluminosilicate</topic><topic>Aluminosilicates</topic><topic>Aluminum silicates</topic><topic>Brownian motion</topic><topic>Colloiding</topic><topic>Condensed Matter</topic><topic>Connectivity</topic><topic>Constitutive models</topic><topic>Frequency analysis</topic><topic>Gelation</topic><topic>Gels</topic><topic>gels and glasses</topic><topic>MATERIALS SCIENCE</topic><topic>Microstructure</topic><topic>Nanoparticles</topic><topic>Physical Sciences</topic><topic>Physics</topic><topic>Relaxation time</topic><topic>relaxation time spectrum</topic><topic>Silica</topic><topic>Silicon dioxide</topic><topic>Soft Condensed Matter</topic><topic>Spectroscopy</topic><topic>Spectrum analysis</topic><topic>Superposition (mathematics)</topic><topic>time-connectivity superposition</topic><topic>Viscoelasticity</topic><topic>weak colloidal gels</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Keshavarz, Bavand</creatorcontrib><creatorcontrib>Rodrigues, Donatien Gomes</creatorcontrib><creatorcontrib>Champenois, Jean-Baptiste</creatorcontrib><creatorcontrib>Frith, Matthew G.</creatorcontrib><creatorcontrib>Ilavsky, Jan</creatorcontrib><creatorcontrib>Geri, Michela</creatorcontrib><creatorcontrib>Divoux, Thibaut</creatorcontrib><creatorcontrib>McKinley, Gareth H.</creatorcontrib><creatorcontrib>Poulesquen, Arnaud</creatorcontrib><creatorcontrib>Argonne National Lab. 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(ANL), Argonne, IL (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Time–connectivity superposition and the gel/glass duality of weak colloidal gels</atitle><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle><addtitle>Proc Natl Acad Sci U S A</addtitle><date>2021-04-13</date><risdate>2021</risdate><volume>118</volume><issue>15</issue><spage>1</spage><epage>9</epage><pages>1-9</pages><issn>0027-8424</issn><eissn>1091-6490</eissn><abstract>Colloidal gels result from the aggregation of Brownian particles suspended in a solvent. Gelation is induced by attractive interactions between individual particles that drive the formation of clusters, which in turn aggregate to form a space-spanning structure. We study this process in aluminosilicate colloidal gels through time-resolved structural and mechanical spectroscopy. Using the time–connectivity superposition principle a series of rapidly acquired linear viscoelastic spectra, measured throughout the gelation process by applying an exponential chirp protocol, are rescaled onto a universal master curve that spans over eight orders of magnitude in reduced frequency. This analysis reveals that the underlying relaxation time spectrum of the colloidal gel is symmetric in time with power-law tails characterized by a single exponent that is set at the gel point. The microstructural mechanical network has a dual character; at short length scales and fast times it appears glassy, whereas at longer times and larger scales it is gel-like. These results can be captured by a simple three-parameter constitutive model and demonstrate that the microstructure of a mature colloidal gel bears the residual skeleton of the original sample-spanning network that is created at the gel point. Our conclusions are confirmed by applying the same technique to another well-known colloidal gel system composed of attractive silica nanoparticles. 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subjects | aluminosilicate Aluminosilicates Aluminum silicates Brownian motion Colloiding Condensed Matter Connectivity Constitutive models Frequency analysis Gelation Gels gels and glasses MATERIALS SCIENCE Microstructure Nanoparticles Physical Sciences Physics Relaxation time relaxation time spectrum Silica Silicon dioxide Soft Condensed Matter Spectroscopy Spectrum analysis Superposition (mathematics) time-connectivity superposition Viscoelasticity weak colloidal gels |
title | Time–connectivity superposition and the gel/glass duality of weak colloidal gels |
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