Pegram Laurel M, Record M Thomas
Department of Biochemistry, University of Wisconsin-Madison, Madison, WI 53706, USA.
J Phys Chem C Nanomater Interfaces. 2009 Feb 12;113(6):2171-2174. doi: 10.1021/jp8073305.
Recently, we developed a quantitative interpretation of surface tension increments (STI) of salts, acids, and bases in terms of the solute (or salt ion) partitioning model (SPM). Here, we obtain an analogous SPM-based interpretation of surface tension increments of nonelectrolytes, which yields local-bulk partition coefficients (K(p)) quantifying the accumulation or exclusion of these solutes in the local region near the air-water surface, and the amount of water per unit area of that region (b1σ). Sucrose exhibits the largest positive STI (approximately 1.4 ergs cm(-2) Osm(-1)). Assuming that K(p) = 0 for sucrose (i.e. that it is completely excluded from the surface of water), these STI provide a minimum estimate of b1σ of 0.20 H(2)O/Å(2), or a minimum thickness of the surface region of approximately two layers of water at bulk density. This is the same value as obtained previously from analysis of surface tension and hydrocarbon solubility increments of Na(2)SO(4) and also for the interaction of glycine betaine with anionic carboxylate surface, indicating that this quantity is not a function of the type of solute or surface investigated and therefore that it may represent the molecular thickness of the region. Partition coefficients of other nonelectrolytes investigated range from moderately excluded (e.g urea) to moderately accumulated (e.g. glycerol, ethylene glycol); strongly accumulated surface active solutes (e.g. mono-substituted alcohols) were not included in this analysis. Partition coefficients for many salt ions obtained from STI and hydrocarbon solubility increments fall in a rank order which corresponds to the Hofmeister series for protein folding and protein solubility, indicating a common pattern of accumulation or exclusion of salt ions at the air-water surface and nonpolar surfaces of dissolved hydrocarbons and proteins; no such patterns are observed for nonelectrolytes.
最近,我们根据溶质(或盐离子)分配模型(SPM)对盐、酸和碱的表面张力增量(STI)进行了定量解释。在此,我们获得了基于SPM的非电解质表面张力增量的类似解释,该解释得出了局部-本体分配系数(K(p)),用于量化这些溶质在空气-水表面附近局部区域的积累或排斥情况,以及该区域每单位面积的水量(b1σ)。蔗糖表现出最大的正STI(约1.4尔格·厘米⁻²·渗透压摩尔⁻¹)。假设蔗糖的K(p)=0(即它完全被排除在水表面之外),这些STI提供了b1σ的最小估计值为0.20 H₂O/Ų,或表面区域的最小厚度约为两层本体密度水的厚度。这与之前通过分析硫酸钠的表面张力和烃类溶解度增量以及甘氨酸甜菜碱与阴离子羧酸盐表面的相互作用所获得的值相同,表明该量不是所研究溶质或表面类型的函数,因此它可能代表该区域的分子厚度。所研究的其他非电解质的分配系数范围从中度排斥(如尿素)到中度积累(如甘油、乙二醇);强积累的表面活性溶质(如单取代醇)未包含在本分析中。从STI和烃类溶解度增量获得的许多盐离子的分配系数按等级顺序排列,这与蛋白质折叠和蛋白质溶解度的霍夫迈斯特序列相对应,表明在空气-水表面以及溶解烃和蛋白质的非极性表面上盐离子存在共同的积累或排斥模式;非电解质未观察到此类模式。