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Equilibrium Janus Drop Topology. 2. A Single Drop in a Spherical Continuous Phase
The equilibrium topology is analyzed of a single Janus drops of oils O1 and O2 in a spherical continuous aqueous phase, W, co-centered with O1. The radius of the O1 oil cap is equal to unity, while that of the oil O2 is varied and the cap centered individually. When the space of O2 exceeds the limit...
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Published in: | Journal of dispersion science and technology 2015-12, Vol.36 (12), p.1685-1692 |
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container_title | Journal of dispersion science and technology |
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creator | Friberg, Stig E. |
description | The equilibrium topology is analyzed of a single Janus drops of oils O1 and O2 in a spherical continuous aqueous phase, W, co-centered with O1. The radius of the O1 oil cap is equal to unity, while that of the oil O2 is varied and the cap centered individually. When the space of O2 exceeds the limit of W, the excess volume is discarded and the border surface of W is considered without interfacial energy. Earlier findings, when increasing the O2 on O1 coverage on a single Janus drop in an infinite aqueous phase, brought to light a selective O2 inversion from an emulsion (O1 + O2)/W to (O1 + W)/O2 at a well-defined surface coverage of O1 by O2. This specific inversion did not take place with the Janus drop in an aqueous phase of limited dimensions. Instead the inversion was perceived to take place, when the volume fraction of O2, V
O2
= (V
O1
+ V
w
+ V
O2
) exceeded 0.5. The information from the earlier publication was used to calculate the variations of volumes V
O2
and V
W
with the radius of the W sphere. The results partially contradicted earlier results. |
doi_str_mv | 10.1080/01932691.2014.1003070 |
format | article |
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O2
= (V
O1
+ V
w
+ V
O2
) exceeded 0.5. The information from the earlier publication was used to calculate the variations of volumes V
O2
and V
W
with the radius of the W sphere. The results partially contradicted earlier results.</description><identifier>ISSN: 0193-2691</identifier><identifier>EISSN: 1532-2351</identifier><identifier>DOI: 10.1080/01932691.2014.1003070</identifier><language>eng</language><publisher>Philadelphia: Taylor & Francis</publisher><subject>Borders ; Dispersions ; Double emulsions ; emulsions drop topology ; interfacial equilibrium ; interfacial tensions ; Inversions ; janus emulsions ; Mathematical analysis ; Nanoparticles ; Topology ; Unity</subject><ispartof>Journal of dispersion science and technology, 2015-12, Vol.36 (12), p.1685-1692</ispartof><rights>Copyright © Taylor & Francis Group, LLC 2015</rights><rights>Copyright © Taylor & Francis Group, LLC</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c408t-37b2025a3b9a1ebf833d0200bfcbe2ab9ca395e59ad2715192e6913de99487a23</citedby><cites>FETCH-LOGICAL-c408t-37b2025a3b9a1ebf833d0200bfcbe2ab9ca395e59ad2715192e6913de99487a23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Friberg, Stig E.</creatorcontrib><title>Equilibrium Janus Drop Topology. 2. A Single Drop in a Spherical Continuous Phase</title><title>Journal of dispersion science and technology</title><description>The equilibrium topology is analyzed of a single Janus drops of oils O1 and O2 in a spherical continuous aqueous phase, W, co-centered with O1. The radius of the O1 oil cap is equal to unity, while that of the oil O2 is varied and the cap centered individually. When the space of O2 exceeds the limit of W, the excess volume is discarded and the border surface of W is considered without interfacial energy. Earlier findings, when increasing the O2 on O1 coverage on a single Janus drop in an infinite aqueous phase, brought to light a selective O2 inversion from an emulsion (O1 + O2)/W to (O1 + W)/O2 at a well-defined surface coverage of O1 by O2. This specific inversion did not take place with the Janus drop in an aqueous phase of limited dimensions. Instead the inversion was perceived to take place, when the volume fraction of O2, V
O2
= (V
O1
+ V
w
+ V
O2
) exceeded 0.5. The information from the earlier publication was used to calculate the variations of volumes V
O2
and V
W
with the radius of the W sphere. The results partially contradicted earlier results.</description><subject>Borders</subject><subject>Dispersions</subject><subject>Double emulsions</subject><subject>emulsions drop topology</subject><subject>interfacial equilibrium</subject><subject>interfacial tensions</subject><subject>Inversions</subject><subject>janus emulsions</subject><subject>Mathematical analysis</subject><subject>Nanoparticles</subject><subject>Topology</subject><subject>Unity</subject><issn>0193-2691</issn><issn>1532-2351</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLAzEUhYMoWKs_QQi4cTP1JplXdpZaXxRUWtchM820KWkyTTpI_70ZqhsXri733u8cDgehawIjAiXcAeGM5pyMKJA0noBBASdoQDJGE8oycooGPZP00Dm6CGEDcS-gHKCP6a7TRlded1v8Km0X8IN3LV641hm3OowwHeExnmu7Mur40hZLPG_XyutaGjxxdq9t56LyfS2DukRnjTRBXf3MIfp8nC4mz8ns7ellMp4ldQrlPmFFRYFmklVcElU1JWNLoABVU1eKyorXkvFMZVwuaUEywqmK6dlScZ6WhaRsiG6Pvq13u06FvdjqUCtjpFUxjCAFKXlUpiyiN3_Qjeu8jekEyXkONC_zLFLZkaq9C8GrRrReb6U_CAKiL1r8Fi36osVP0VF3f9Rp2zi_lV_Om6XYy4NxvvHS1joI9r_FN9S8ggE</recordid><startdate>20151202</startdate><enddate>20151202</enddate><creator>Friberg, Stig E.</creator><general>Taylor & Francis</general><general>Taylor & Francis Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20151202</creationdate><title>Equilibrium Janus Drop Topology. 2. A Single Drop in a Spherical Continuous Phase</title><author>Friberg, Stig E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c408t-37b2025a3b9a1ebf833d0200bfcbe2ab9ca395e59ad2715192e6913de99487a23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Borders</topic><topic>Dispersions</topic><topic>Double emulsions</topic><topic>emulsions drop topology</topic><topic>interfacial equilibrium</topic><topic>interfacial tensions</topic><topic>Inversions</topic><topic>janus emulsions</topic><topic>Mathematical analysis</topic><topic>Nanoparticles</topic><topic>Topology</topic><topic>Unity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Friberg, Stig E.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of dispersion science and technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Friberg, Stig E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Equilibrium Janus Drop Topology. 2. A Single Drop in a Spherical Continuous Phase</atitle><jtitle>Journal of dispersion science and technology</jtitle><date>2015-12-02</date><risdate>2015</risdate><volume>36</volume><issue>12</issue><spage>1685</spage><epage>1692</epage><pages>1685-1692</pages><issn>0193-2691</issn><eissn>1532-2351</eissn><abstract>The equilibrium topology is analyzed of a single Janus drops of oils O1 and O2 in a spherical continuous aqueous phase, W, co-centered with O1. The radius of the O1 oil cap is equal to unity, while that of the oil O2 is varied and the cap centered individually. When the space of O2 exceeds the limit of W, the excess volume is discarded and the border surface of W is considered without interfacial energy. Earlier findings, when increasing the O2 on O1 coverage on a single Janus drop in an infinite aqueous phase, brought to light a selective O2 inversion from an emulsion (O1 + O2)/W to (O1 + W)/O2 at a well-defined surface coverage of O1 by O2. This specific inversion did not take place with the Janus drop in an aqueous phase of limited dimensions. Instead the inversion was perceived to take place, when the volume fraction of O2, V
O2
= (V
O1
+ V
w
+ V
O2
) exceeded 0.5. The information from the earlier publication was used to calculate the variations of volumes V
O2
and V
W
with the radius of the W sphere. The results partially contradicted earlier results.</abstract><cop>Philadelphia</cop><pub>Taylor & Francis</pub><doi>10.1080/01932691.2014.1003070</doi><tpages>8</tpages></addata></record> |
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language | eng |
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source | Taylor and Francis Science and Technology Collection |
subjects | Borders Dispersions Double emulsions emulsions drop topology interfacial equilibrium interfacial tensions Inversions janus emulsions Mathematical analysis Nanoparticles Topology Unity |
title | Equilibrium Janus Drop Topology. 2. A Single Drop in a Spherical Continuous Phase |
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