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界面水中非线性介电响应的极性依赖性。

Polarity-dependence of the nonlinear dielectric response in interfacial water.

机构信息

Department of Chemistry, Virginia Commonwealth University, Richmond, Virginia 23221, USA.

出版信息

J Chem Phys. 2023 Apr 7;158(13):134716. doi: 10.1063/5.0142483.

DOI:10.1063/5.0142483
PMID:37031102
Abstract

Molecular dynamics simulations are used to study the nonlinear dielectric responses of a confined aqueous film in a planar nanopore under perpendicular electric fields at varied voltages between confining graphene sheets. Dielectric saturation reminiscent of the bulk phase behavior is prevalent at very strong fields, whereas we observe a nonmonotonic permittivity dependence on the electric field at intermediate strengths where field-alignment and spontaneous polarization of interfacial water are of comparable magnitude. The coupling between the two effects results in distinct dielectric responses at opposite confinement walls. The normal component of both the differential dielectric constant and dielectric difference constant tensors averaged over the region closer to the wall under an incoming electric field (field pointing from the liquid to the solid phase) initially increases with the strength of the imposed field. The differential permittivity peaks at a field strength previously shown to offset the surface-induced orientation bias of hydration molecules at this wall. Further strengthening of the field results in a conventional saturation behavior. At the opposite wall (subject to outgoing field) and in the central region of the water slab, the nonlinear dielectric response resembles bulklike saturation. The conditions at the permittivity extremum coincide with the window of accelerated reorientation rates of interfacial water molecules under an incoming field we uncovered in earlier molecular dynamics analyses.

摘要

采用分子动力学模拟研究了在垂直电场中受限的水膜在两个石墨烯片之间的平面纳米孔中的非线性介电响应。在非常强的场下,普遍存在类似于体相行为的介电饱和现象,而在中等强度下,我们观察到介电常数与电场呈非单调依赖关系,此时界面水分子的场取向和自发极化具有相当的大小。这两种效应的耦合导致在相反的限制壁处具有不同的介电响应。在一个外加电场下(从液体指向固体相),靠近壁的区域的差分介电常数和介电差常数张量的法向分量的平均值,最初随外加场的强度增加而增加。差分介电常数在以前的研究中已经表明可以抵消该壁上水合分子的表面诱导取向偏置的场强处达到峰值。进一步增强电场会导致常规的饱和行为。在相反的壁(受到外场作用)和水片的中心区域,非线性介电响应类似于块状饱和。在介电常数极值处的条件与我们在早期分子动力学分析中发现的界面水分子在入射场下加速重取向速率的窗口相吻合。

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