How Is the Surface Tension of Various Liquids Distributed along the Interface Normal?

被引:36
作者
Sega, Marcello [1 ]
Fabian, Balazs [2 ,3 ]
Horvai, George [2 ,4 ]
Jedlovszky, Pal [4 ,5 ]
机构
[1] Univ Vienna, Computat Phys Grp, Sensengasse 8-9, A-1090 Vienna, Austria
[2] Budapest Univ Technol & Econ, Dept Inorgan & Analyt Chem, Szt Gellert Ter 4, H-1111 Budapest, Hungary
[3] Univ Bourgogne Franche Comte, Inst UTINAM CNRS UMR 6213, 16 Route Gray, F-25030 Besancon, France
[4] MTA BME Res Grp Tech Analyt Chem, Szt Gellert Ter 4, H-1111 Budapest, Hungary
[5] Eszterhazy Karoly Univ, Dept Chem, Leanyka Utca 6, H-3300 Eger, Hungary
关键词
PARTICLE MESH EWALD; MOLECULAR-DYNAMICS; COMPUTER-SIMULATIONS; INTRINSIC ANALYSIS; METHANOL MIXTURES; VAPOR INTERFACE; WATER; PROFILE; SUMS;
D O I
10.1021/acs.jpcc.6b09880
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The tangential pressure profile has been calculated across the liquid vapor interface of five molecular liquids, i.e., CCl4, acetone, acetonitrile, methanol, and water, in molecular dynamics simulations using a recently developed method. Because the value of the surface tension is directly related to the integral of this profile, the obtained results can be interpreted in terms of the distribution of the surface tension along the interface normal, both as a function of distance, either from the Gibbs dividing surface or from the capillary wave corrugated real, intrinsic liquid surface, and also in a layerwise manner. The obtained results show that the surface tension is distributed in a 1-2 nm wide range along the interface normal, and at least 85% of its value comes from the first molecular layer of the liquid in every case. The remaining, roughly 10% contribution comes from the second layer, with the exception of methanol, in which the entire surface tension can be accounted for by the first molecular layer. Contributions of the third and subsequent molecular layers are found to be already negligible in every case.
引用
收藏
页码:27468 / 27477
页数:10
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