首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >VAN-DER-WAALS-INTERACTION, SURFACE FREE ENERGIES, AND CONTACT ANGLES - DISPERSIVE POLYMERS AND LIQUIDS
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VAN-DER-WAALS-INTERACTION, SURFACE FREE ENERGIES, AND CONTACT ANGLES - DISPERSIVE POLYMERS AND LIQUIDS

机译:范德华相互作用,表面自由能和接触角-分散性聚合物和液体

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The Lifshitz theory of van der Waals interaction has been employed to calculate the contact angles of diiodomethane, 1-bromonaphthalene, 1-methylnaphthalene, bromobenzene, 1-tert-butylnaphthalene, liquid paraffin, and hexadecane on poly(dimethylsiloxane), poly(4-methyl-1-pentene), polyethylene, natural rubber, and polystyrene surfaces. The theoretical treatment is based on the equation cos theta = [(2A(PVI)/A(LVL))(H-oLVI/H-oPVL)(2)] - 1, where theta is the contact angle and A(PVL) and A(LVL) are the non-retarded Hamaker constants for the heterointeraction between polymer and liquid across vacuum and the homo interaction of the liquid across vacuum, respectively. Nonretarded Hamaker constants have been determined from the dielectric properties of the materials and application of the Lifshitz theory. H-oLVL and H-oPVL are the equilibrium ''contact'' surface separations associated with the Liquid-liquid homointeraction and polymer-liquid heterointeraction across vacuum, respectively. H-oLVL values, and the analogous H-oPVP values associated with polymer homointeraction, have been estimated from the surface free energies of the dispersive liquids and polymers. Four different approaches, each with a different assumption regarding the heterointeraction between polymer and liquid, have been used to obtain H-oPVL values: (i) H-oPVL = H-oLVL, (ii) H-oPVL = H-oPVP, (iii) a geometric mean relationship, H-oPVL = (HoPVPHoLVL)(1/2), and (iv) an arithmetic mean relationship, H-oPVL = (H-oPVP + H-oLVL)/2. Theoretical contact angles obtained with the four approaches have been compared with experimental contact angles. In general, the approaches which employ the combining rules, whether geometric or arithmetic, provide the best agreement between theory and experiment. Previous work that has dealt with the contact angles of n-alkanes on poly(tetrafluoroethylene) has also been reexamined. For the perfluorocarbon-hydrocarbon system none of the approaches are able to reconcile theory and experiment. [References: 51]
机译:范德华相互作用的Lifshitz理论已用于计算二碘甲烷,1-溴萘,1-甲基萘,溴苯,1-叔丁基萘,液体石蜡和十六烷在聚二甲基硅氧烷,聚(4-甲基-1-戊烯),聚乙烯,天然橡胶和聚苯乙烯表面。理论处理基于方程cosθ= [(2A(PVI)/ A(LVL))(H-oLVI / H-oPVL)(2)]-1,其中θ是接触角,A(PVL) A和LV(L L)分别是聚合物和液体在真空中的异质相互作用和液体在真空中的均质相互作用的非延迟Hamaker常数。已根据材料的介电特性和Lifshitz理论的应用确定了非延迟Hamaker常数。 H-oLVL和H-oPVL分别是平衡的``接触''表面分离,分别与整个真空中的液-液均相作用和聚合物-液的杂相作用有关。 H-oLVL值以及与聚合物均相作用相关的类似H-oPVP值已从分散液体和聚合物的表面自由能中估算出来。已使用四种不同的方法来获得H-oPVL值,每种方法都对聚合物和液体之间的杂相互作用有不同的假设:(i)H-oPVL = H-oLVL,(ii)H-oPVL = H-oPVP,( iii)几何平均关系H-oPVL =(HoPVPHoLVL)(1/2),以及(iv)算术平均关系H-oPVL =(H-oPVP + H-oLVL)/ 2。将四种方法获得的理论接触角与实验接触角进行了比较。通常,采用几何或算术组合规则的方法在理论和实验之间提供了最佳的一致性。还研究了处理正构烷烃在聚四氟乙烯上的接触角的先前工作。对于全氟化碳-碳氢化合物系统,这些方法都无法协调理论和实验。 [参考:51]

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