000009450 001__ 9450 000009450 005__ 20240610120050.0 000009450 017__ $$aThis version is available at the following Publisher URL: http://jcp.aip.org 000009450 0247_ $$2DOI$$a10.1063/1.1502242 000009450 0247_ $$2WOS$$aWOS:000178317300044 000009450 0247_ $$2Handle$$a2128/1468 000009450 037__ $$aPreJuSER-9450 000009450 041__ $$aeng 000009450 082__ $$a540 000009450 084__ $$2WoS$$aPhysics, Atomic, Molecular & Chemical 000009450 1001_ $$0P:(DE-Juel1)VDB1412$$aSchilling, T.$$b0$$uFZJ 000009450 245__ $$aWetting in ternary mixtures - with and without amphiphiles 000009450 260__ $$aMelville, NY$$bAmerican Institute of Physics$$c2002 000009450 300__ $$a7284 - 7294 000009450 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000009450 3367_ $$2DataCite$$aOutput Types/Journal article 000009450 3367_ $$00$$2EndNote$$aJournal Article 000009450 3367_ $$2BibTeX$$aARTICLE 000009450 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000009450 3367_ $$2DRIVER$$aarticle 000009450 440_0 $$03145$$aJournal of Chemical Physics$$v117$$x0021-9606 000009450 500__ $$aRecord converted from VDB: 12.11.2012 000009450 520__ $$aThe interfacial wetting behavior of ternary fluid mixtures is investigated, both for systems where all components have isotropic interaction potentials, as well as for systems where one component is an amphiphile. The BEG model and the corresponding two-order-parameter Ginzburg-Landau model are employed for systems without amphiphiles. We calculate the global wetting phase diagram for nonamphiphilic mixtures. In the investigated range of interaction parameters, the wetting transitions are always continuous at three-phase coexistence. The critical behavior is found to be universal in some, nonuniversal in other parts of the phase diagram. For systems with amphiphiles, two additional interaction terms are taken into account. The first models the aggregation of amphiphilic molecules at the air-water interface, the second the formation of amphiphilic bilayers in water. We find that the first term leads to a reduction of the tension of the air-water interface, and favors wetting by the water-rich phase, while the second-bilayer-term leads to a reduction of the tension of the interface between the water-rich and amphiphile-rich phases. (C) 2002 American Institute of Physics. 000009450 536__ $$0G:(DE-Juel1)FUEK242$$2G:(DE-HGF)$$aKondensierte Materie$$cM02$$x0 000009450 588__ $$aDataset connected to Web of Science 000009450 650_7 $$2WoSType$$aJ 000009450 7001_ $$0P:(DE-Juel1)130665$$aGompper, G.$$b1$$uFZJ 000009450 773__ $$0PERI:(DE-600)1473050-9$$a10.1063/1.1502242$$gVol. 117, p. 7284 - 7294$$p7284 - 7294$$q117<7284 - 7294$$tThe @journal of chemical physics$$v117$$x0021-9606$$y2002 000009450 8564_ $$uhttps://juser.fz-juelich.de/record/9450/files/11924.pdf$$yOpenAccess 000009450 8564_ $$uhttps://juser.fz-juelich.de/record/9450/files/11924.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess 000009450 8564_ $$uhttps://juser.fz-juelich.de/record/9450/files/11924.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000009450 8564_ $$uhttps://juser.fz-juelich.de/record/9450/files/11924.jpg?subformat=icon-640$$xicon-640$$yOpenAccess 000009450 909CO $$ooai:juser.fz-juelich.de:9450$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire 000009450 9131_ $$0G:(DE-Juel1)FUEK242$$bMaterie$$kM02$$lKondensierte Materie$$vKondensierte Materie$$x0 000009450 9141_ $$y2002 000009450 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed 000009450 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000009450 9201_ $$0I:(DE-Juel1)VDB31$$d31.12.2006$$gIFF$$kIFF-TH-II$$lTheorie II$$x0 000009450 970__ $$aVDB:(DE-Juel1)11924 000009450 9801_ $$aFullTexts 000009450 980__ $$aVDB 000009450 980__ $$aJUWEL 000009450 980__ $$aConvertedRecord 000009450 980__ $$ajournal 000009450 980__ $$aI:(DE-Juel1)ICS-2-20110106 000009450 980__ $$aUNRESTRICTED 000009450 980__ $$aFullTexts 000009450 981__ $$aI:(DE-Juel1)IBI-5-20200312 000009450 981__ $$aI:(DE-Juel1)IAS-2-20090406 000009450 981__ $$aI:(DE-Juel1)ICS-2-20110106