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本文引用的文献

1
Evaluation of B3LYP, X3LYP, and M06-Class Density Functionals for Predicting the Binding Energies of Neutral, Protonated, and Deprotonated Water Clusters.用于预测中性、质子化和去质子化水团簇结合能的B3LYP、X3LYP和M06类密度泛函的评估。
J Chem Theory Comput. 2009 Apr 14;5(4):1016-26. doi: 10.1021/ct800549f. Epub 2009 Mar 12.
2
New Insights into the Structure of the Vapor/Water Interface from Large-Scale First-Principles Simulations.基于大规模第一性原理模拟对汽/水界面结构的新认识
J Phys Chem Lett. 2011 Jan 20;2(2):105-13. doi: 10.1021/jz101391r. Epub 2010 Dec 30.
3
Unveiling Electron Promiscuity.揭示电子的混乱行为
J Phys Chem Lett. 2011 May 19;2(10):1216-22. doi: 10.1021/jz2002875. Epub 2011 May 3.
4
Quantifying accumulation or exclusion of H, HO, and Hofmeister salt ions near interfaces.量化H⁺、OH⁻和霍夫迈斯特盐离子在界面附近的聚集或排斥情况。
Chem Phys Lett. 2008 Dec;467(1-3):1-8. doi: 10.1016/j.cplett.2008.10.090.
5
Anions dramatically enhance proton transfer through aqueous interfaces.阴离子显著增强质子穿过水相界面的传递。
Proc Natl Acad Sci U S A. 2012 Jun 26;109(26):10228-32. doi: 10.1073/pnas.1200949109. Epub 2012 Jun 11.
6
Speed limits for acid-base chemistry in aqueous solutions.水溶液中酸碱化学的速率限制。
Chimia (Aarau). 2012;66(4):182-6. doi: 10.2533/chimia.2012.182.
7
The surface relaxation of water.水的表面弛豫。
J Phys Chem B. 2012 Aug 2;116(30):8981-8. doi: 10.1021/jp211810v. Epub 2012 Jul 12.
8
Hofmeister effects in micromolar electrolyte solutions.微摩尔电解质溶液中的贺夫迈斯特效应。
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9
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10
Elucidating the mechanism of selective ion adsorption to the liquid water surface.阐明选择性离子吸附到液态水表面的机制。
Proc Natl Acad Sci U S A. 2012 Jan 17;109(3):701-5. doi: 10.1073/pnas.1116169109. Epub 2012 Jan 10.

气-水界面的布朗斯特碱性。

Brønsted basicity of the air-water interface.

机构信息

Ronald and Maxine Linde Center for Global Environmental Science, Materials Science Department, California Institute of Technology, Pasadena, CA 91125, USA.

出版信息

Proc Natl Acad Sci U S A. 2012 Nov 13;109(46):18679-83. doi: 10.1073/pnas.1209307109. Epub 2012 Oct 29.

DOI:10.1073/pnas.1209307109
PMID:23112167
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3503180/
Abstract

Differences in the extent of protonation of functional groups lying on either side of water-hydrophobe interfaces are deemed essential to enzymatic catalysis, molecular recognition, bioenergetic transduction, and atmospheric aerosol-gas exchanges. The sign and range of such differences, however, remain conjectural. Herein we report experiments showing that gaseous carboxylic acids RCOOH(g) begin to deprotonate on the surface of water significantly more acidic than that supporting the dissociation of dissolved acids RCOOH(aq). Thermodynamic analysis indicates that > 6 H(2)O molecules must participate in the deprotonation of RCOOH(g) on water, but quantum mechanical calculations on a model air-water interface predict that such event is hindered by a significant kinetic barrier unless OH(-) ions are present therein. Thus, by detecting RCOO(-) we demonstrate the presence of OH(-) on the aerial side of on pH > 2 water exposed to RCOOH(g). Furthermore, because in similar experiments the base (Me)(3)N(g) is protonated only on pH < 4 water, we infer that the outer surface of water is Brønsted neutral at pH ∼3 (rather than at pH 7 as bulk water), a value that matches the isoelectric point of bubbles and oil droplets in independent electrophoretic experiments. The OH(-) densities sensed by RCOOH(g) on the aerial surface of water, however, are considerably smaller than those at the (>1 nm) deeper shear planes probed in electrophoresis, thereby implying the existence of OH(-) gradients in the interfacial region. This fact could account for the weak OH(-) signals detected by surface-specific spectroscopies.

摘要

位于水-疏水分子界面两侧的官能团的质子化程度的差异被认为对酶催化、分子识别、生物能量传递和大气气溶胶-气体交换至关重要。然而,这些差异的符号和范围仍然是推测性的。本文报道的实验表明,气态羧酸 RCOOH(g) 在水表面开始去质子化的酸度显著低于支持溶解酸 RCOOH(aq) 离解的酸度。热力学分析表明,在水中 RCOOH(g) 的去质子化过程中必须有超过 6 个 H₂O 分子参与,但在空气-水界面的模型上的量子力学计算预测,除非存在 OH⁻离子,否则这种情况会受到显著的动力学障碍的阻碍。因此,通过检测 RCOO⁻,我们证明了在 pH 值大于 2 的水暴露于 RCOOH(g) 的空气侧存在 OH⁻。此外,由于在类似的实验中,碱(Me)₃N(g)仅在 pH < 4 的水中质子化,我们推断水的外表面在 pH ≈ 3 时是布朗斯台德中性的(而不是在 pH 7 时是 bulk water),这一值与独立电泳实验中气泡和油滴的等电点相匹配。然而,RCOOH(g) 在水的空气侧表面感应到的 OH⁻密度明显小于电泳中探测到的(>1nm)更深的剪切平面的密度,这意味着在界面区域存在 OH⁻梯度。这一事实可以解释表面特异性光谱学检测到的弱 OH⁻信号。