Spontaneous Mosaics of Charge Formed by Liquid Evaporation
Commonly used liquids have a powerful effect on producing electrostatic patterns in dielectric surfaces. During evaporation, charges are built‐up on dielectric surfaces that support liquids but with an important difference: negative charges appear where the liquid evaporates while positive ones are...
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Veröffentlicht in: | Advanced materials interfaces 2020-09, Vol.7 (18), p.n/a |
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description | Commonly used liquids have a powerful effect on producing electrostatic patterns in dielectric surfaces. During evaporation, charges are built‐up on dielectric surfaces that support liquids but with an important difference: negative charges appear where the liquid evaporates while positive ones are formed within the residual liquid. After complete evaporation, the result is a mosaic of stable and fixed surface charges resulting in electrostatic potential gradients as large as 20 kV m−1, but charge partitioning can be suppressed with common surfactants. The results can be understood considering the Maxwell–Wagner effect where charge accumulation takes place during current flowing across the interface. All these findings help to explain the hitherto challenging problem of static electricity and the appearance of the ubiquitous electrostatic patterns in dielectrics, what it must be helpful for the controlling of electrostatic charges in industry or in common laboratory activities.
Unprecedent results show that during the evaporation of common liquids, large positive and negative charge domains are naturally formed at the interface as the result of charge partition during phase transition. Charges are accumulated within the bulk liquid while negative charges are built‐up at the liquid–solid–air interface, resulting in a multipolar electret that can be understood considering the Maxwell–Wagner effect. |
doi_str_mv | 10.1002/admi.202000884 |
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Unprecedent results show that during the evaporation of common liquids, large positive and negative charge domains are naturally formed at the interface as the result of charge partition during phase transition. Charges are accumulated within the bulk liquid while negative charges are built‐up at the liquid–solid–air interface, resulting in a multipolar electret that can be understood considering the Maxwell–Wagner effect.</description><identifier>ISSN: 2196-7350</identifier><identifier>EISSN: 2196-7350</identifier><identifier>DOI: 10.1002/admi.202000884</identifier><language>eng</language><publisher>Weinheim: John Wiley & Sons, Inc</publisher><subject>contact charging ; Dielectrics ; electrostatic mapping ; Kelvin probe ; liquid evaporation ; Liquids ; mosaic of charges ; Mosaics ; Potential gradient ; Static electricity</subject><ispartof>Advanced materials interfaces, 2020-09, Vol.7 (18), p.n/a</ispartof><rights>2020 Wiley‐VCH GmbH</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3174-402f4d4f714500f699b2071b14720bb73ccc4e7185b1bf22bc2508c361b9a7733</citedby><cites>FETCH-LOGICAL-c3174-402f4d4f714500f699b2071b14720bb73ccc4e7185b1bf22bc2508c361b9a7733</cites><orcidid>0000-0003-2521-3574</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fadmi.202000884$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fadmi.202000884$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27923,27924,45573,45574</link.rule.ids></links><search><creatorcontrib>Moreira, Kelly S.</creatorcontrib><creatorcontrib>Lermen, Diana</creatorcontrib><creatorcontrib>Campo, Yan A. Santos</creatorcontrib><creatorcontrib>Ferreira, Leticia O.</creatorcontrib><creatorcontrib>Burgo, Thiago A. L.</creatorcontrib><title>Spontaneous Mosaics of Charge Formed by Liquid Evaporation</title><title>Advanced materials interfaces</title><description>Commonly used liquids have a powerful effect on producing electrostatic patterns in dielectric surfaces. During evaporation, charges are built‐up on dielectric surfaces that support liquids but with an important difference: negative charges appear where the liquid evaporates while positive ones are formed within the residual liquid. After complete evaporation, the result is a mosaic of stable and fixed surface charges resulting in electrostatic potential gradients as large as 20 kV m−1, but charge partitioning can be suppressed with common surfactants. The results can be understood considering the Maxwell–Wagner effect where charge accumulation takes place during current flowing across the interface. All these findings help to explain the hitherto challenging problem of static electricity and the appearance of the ubiquitous electrostatic patterns in dielectrics, what it must be helpful for the controlling of electrostatic charges in industry or in common laboratory activities.
Unprecedent results show that during the evaporation of common liquids, large positive and negative charge domains are naturally formed at the interface as the result of charge partition during phase transition. Charges are accumulated within the bulk liquid while negative charges are built‐up at the liquid–solid–air interface, resulting in a multipolar electret that can be understood considering the Maxwell–Wagner effect.</description><subject>contact charging</subject><subject>Dielectrics</subject><subject>electrostatic mapping</subject><subject>Kelvin probe</subject><subject>liquid evaporation</subject><subject>Liquids</subject><subject>mosaic of charges</subject><subject>Mosaics</subject><subject>Potential gradient</subject><subject>Static electricity</subject><issn>2196-7350</issn><issn>2196-7350</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNqFkD1PwzAQQC0EElXpymyJOeX8kTphq0oLlVoxALNlOza4auPUbkD596QqAjamu-G9O-khdE1gTADorap2fkyBAkBR8DM0oKScZILlcP5nv0SjlDY9QwgltGADdPfchPqgahvahNchKW8SDg7P3lV8s3gR4s5WWHd45fetr_D8QzUhqoMP9RW6cGqb7Oh7DtHrYv4ye8xWTw_L2XSVGUYEzzhQxyvuBOE5gJuUpaYgiCZcUNBaMGMMt4IUuSbaUaoNzaEwbEJ0qYRgbIhuTnebGPatTQe5CW2s-5eScp4XQpQcemp8okwMKUXrZBP9TsVOEpDHRPKYSP4k6oXyJHz6re3-oeX0fr38db8ABiRoCg</recordid><startdate>20200901</startdate><enddate>20200901</enddate><creator>Moreira, Kelly S.</creator><creator>Lermen, Diana</creator><creator>Campo, Yan A. Santos</creator><creator>Ferreira, Leticia O.</creator><creator>Burgo, Thiago A. L.</creator><general>John Wiley & Sons, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-2521-3574</orcidid></search><sort><creationdate>20200901</creationdate><title>Spontaneous Mosaics of Charge Formed by Liquid Evaporation</title><author>Moreira, Kelly S. ; Lermen, Diana ; Campo, Yan A. Santos ; Ferreira, Leticia O. ; Burgo, Thiago A. L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3174-402f4d4f714500f699b2071b14720bb73ccc4e7185b1bf22bc2508c361b9a7733</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>contact charging</topic><topic>Dielectrics</topic><topic>electrostatic mapping</topic><topic>Kelvin probe</topic><topic>liquid evaporation</topic><topic>Liquids</topic><topic>mosaic of charges</topic><topic>Mosaics</topic><topic>Potential gradient</topic><topic>Static electricity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Moreira, Kelly S.</creatorcontrib><creatorcontrib>Lermen, Diana</creatorcontrib><creatorcontrib>Campo, Yan A. Santos</creatorcontrib><creatorcontrib>Ferreira, Leticia O.</creatorcontrib><creatorcontrib>Burgo, Thiago A. L.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Advanced materials interfaces</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Moreira, Kelly S.</au><au>Lermen, Diana</au><au>Campo, Yan A. Santos</au><au>Ferreira, Leticia O.</au><au>Burgo, Thiago A. L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spontaneous Mosaics of Charge Formed by Liquid Evaporation</atitle><jtitle>Advanced materials interfaces</jtitle><date>2020-09-01</date><risdate>2020</risdate><volume>7</volume><issue>18</issue><epage>n/a</epage><issn>2196-7350</issn><eissn>2196-7350</eissn><abstract>Commonly used liquids have a powerful effect on producing electrostatic patterns in dielectric surfaces. During evaporation, charges are built‐up on dielectric surfaces that support liquids but with an important difference: negative charges appear where the liquid evaporates while positive ones are formed within the residual liquid. After complete evaporation, the result is a mosaic of stable and fixed surface charges resulting in electrostatic potential gradients as large as 20 kV m−1, but charge partitioning can be suppressed with common surfactants. The results can be understood considering the Maxwell–Wagner effect where charge accumulation takes place during current flowing across the interface. All these findings help to explain the hitherto challenging problem of static electricity and the appearance of the ubiquitous electrostatic patterns in dielectrics, what it must be helpful for the controlling of electrostatic charges in industry or in common laboratory activities.
Unprecedent results show that during the evaporation of common liquids, large positive and negative charge domains are naturally formed at the interface as the result of charge partition during phase transition. Charges are accumulated within the bulk liquid while negative charges are built‐up at the liquid–solid–air interface, resulting in a multipolar electret that can be understood considering the Maxwell–Wagner effect.</abstract><cop>Weinheim</cop><pub>John Wiley & Sons, Inc</pub><doi>10.1002/admi.202000884</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0003-2521-3574</orcidid></addata></record> |
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subjects | contact charging Dielectrics electrostatic mapping Kelvin probe liquid evaporation Liquids mosaic of charges Mosaics Potential gradient Static electricity |
title | Spontaneous Mosaics of Charge Formed by Liquid Evaporation |
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