首页> 美国卫生研究院文献>The Journal of Chemical Physics >Molecular dynamics simulations of nonpolarizable inorganic salt solution interfaces: NaCl NaBr and NaI in transferable intermolecular potential 4-point with charge dependent polarizability (TIP4P-QDP) water
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Molecular dynamics simulations of nonpolarizable inorganic salt solution interfaces: NaCl NaBr and NaI in transferable intermolecular potential 4-point with charge dependent polarizability (TIP4P-QDP) water

机译:不可极化的无机盐溶液界面:NaClNaBr和NaI在可转移的分子间电势4点中具有电荷依赖性极化率(TIP4P-QDP)的分子动力学模拟

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摘要

We present molecular dynamics simulations of the liquid-vapor interface of 1M salt solutions of nonpolarizable NaCl, NaBr, and NaI in polarizable transferable intermolecular potential 4-point with charge dependent polarizability water []; this water model accommodates increased solvent polarizability (relative to the condensed phase) in the interfacial and vapor regions. We employ fixed-charge ion models developed in conjunction with the TIP4P-QDP water model to reproduce ab initio ion-water binding energies and ion-water distances for isolated ion-water pairs. The transferability of these ion models to the condensed phase was validated with hydration free energies computed using thermodynamic integration (TI) and appropriate energy corrections. Density profiles of Cl, Br, and I exhibit charge layering in the interfacial region; anions and cation interfacial probabilities show marked localization, with the anions penetrating further toward the vapor than the cations. Importantly, in none of the cases studied do anions favor the outermost regions of the interface; there is always an aqueous region between the anions and vapor phase. Observed interfacial charge layering is independent of the strength of anion-cation interactions as manifest in anion-cation contact ion pair peaks and solvent separated ion pair peaks; by artificially modulating the strength of anion-cation interactions (independent of their interactions with solvent), we find little dependence on charge layering particularly for the larger iodide anion. The present results reiterate the widely held view of the importance of solvent and ion polarizability in mediating specific anion surface segregation effects. Moreover, due to the higher parametrized polarizability of the TIP4P-QDP condensed phase {1.31 Å3 for TIP4P-QDP versus 1.1 Å3 (TIP4P-FQ) and 0.87 Å3 (POL3) []} based on ab initio calculations of the condensed-phase polarizability reduction in liquid water, the present simulations highlight the role of water polarizability in inducing water molecular dipole moments parallel to the interface normal (and within the interfacial region) so as to favorably oppose the macrodipole generated by the separation of anion and cation charge. Since the TIP4P-QDP water polarizability approaches that of the experimental vapor phase value for water, the present results suggest a fundamental role of solvent polarizability in accommodating the large spatial dipole generated by the separation of ion charges. The present results draw further attention to the question of what exact value of condensed phase water polarizability to incorporate in classical polarizable water force fields.
机译:我们提供了分子动力学模拟,模拟了不可极化的NaCl,NaBr和NaI的1M盐溶液在极化可转移的分子间电势4点中的电荷依赖性极化水[]。该水模型可在界面和蒸汽区域适应增加的溶剂极化率(相对于冷凝相)。我们采用与TIP4P-QDP水模型结合开发的固定电荷离子模型来重现从头开始的离子水结合能和离析的离子水对的离子水距离。使用热力学积分(TI)和适当的能量校正计算得出的水合自由能验证了这些离子模型向凝聚相的转移能力。 Cl -,Br -和I -的密度分布在界面区域显示出电荷分层。阴离子和阳离子的界面概率显示出显着的局部性,其中阴离子比阳离子更向蒸气渗透。重要的是,在所研究的任何情况下,阴离子都不会偏向界面的最外层区域。在阴离子和气相之间始终存在一个水相区域。观察到的界面电荷分层与阴离子-阳离子相互作用的强度无关,这表现在阴离子-阳离子接触离子对峰和溶剂分离的离子对峰中。通过人为调节阴离子-阳离子相互作用的强度(独立于它们与溶剂的相互作用),我们发现对电荷分层的依赖性很小,尤其是对于较大的碘化物阴离子而言。本结果重申了溶剂和离子极化度在介导特定阴离子表面偏析效应中的重要性的广泛观点。此外,由于TIP4P-QDP凝聚相的参量极化率较高(TIP4P-QDP为{1.31Å 3 ),相对于1.1Å 3 (TIP4P-FQ)和0.87Å< sup> 3 (POL3)[]}基于液态水中冷凝相极化率降低的从头算,本模拟突出了水极化率在诱导平行于界面法线的水分子偶极矩中的作用(并在界面区域内),以有利地抵抗由阴离子和阳离子电荷的分离产生的大偶极子。由于TIP4P-QDP的水极化率接近水的实验气相值,因此本结果表明溶剂极化率在适应由离子电荷分离产生的大空间偶极子方面的基本作用。目前的结果使人们进一步关注以下问题:在经典的可极化水力场中应包含什么凝相水极化率的精确值。

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