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首页> 外文期刊>The Journal of Chemical Physics >Rigidity and soft percolation in the glass transition of an atomistic model of ionic liquid, 1-ethyl-3-methyl imidazolium nitrate, from molecular dynamics simulations-Existence of infinite overlapping networks in a fragile ionic liquid
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Rigidity and soft percolation in the glass transition of an atomistic model of ionic liquid, 1-ethyl-3-methyl imidazolium nitrate, from molecular dynamics simulations-Existence of infinite overlapping networks in a fragile ionic liquid

机译:离子液体1-乙基-3-甲基咪唑鎓硝酸盐的原子模型在玻璃化转变中的刚性和软渗透-来自分子动力学模拟-脆弱离子液体中无限重叠网络的存在

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摘要

The typical ionic liquid, 1-ethyl-3-methyl imidazolium nitrate (EMIM-NO3), was examined by molecular dynamics simulations of an all-atomistic model to show the characteristics of networks of cages and/or bonds in the course of vitrification of this fragile glass-former. The system shows changes of dynamics at two characteristic temperatures, T-B (or T-c) and the glass transition temperature T-g, found in other fragile glass forming liquids [K. L. Ngai and J. Habasaki, J. Chem. Phys. 141, 114502 (2014)]. On decreasing temperature, the number of neighboring cation-anion pairs, N-B, within the first minimum of the pair correlation function, g(r)(min), increases. On crossing T-B (>T-g), the system volume and diffusion coefficient both show changes in temperature dependence, and as usual at T-g. The glass transition temperature, T-g, is characterized by the saturation of the total number of "bonds," N-B and the corresponding decrease in degree of freedom, F = [(3N - 6) - N-B], of the system consisting of N particles. Similar behavior holds for the other ion-ion pairs. Therefore, as an alternative, the dynamics of glass transition can be interpreted conceptually by rigidity percolation. Before saturation occurring at T-g, the number of bonds shows a remarkable change at around T-B. This temperature is associated with the disappearance of the loosely packed coordination polyhedra of anions around cation (or vice versa), related to the loss of geometrical freedom of the polyhedra, f(g), of each coordination polyhedron, which can be defined by f(g) = [(3N(V) - 6) - N-b]. Here, 3N(v) is the degree of freedom of N-V vertices of the polyhedron, and N-b is number of fictive bonds. The packing of polyhedra is characterized by the soft percolation of cages, which allows further changes with decreasing temperature. The power spectrum of displacement of the central ion in the cage is found to be correlated with the fluctuation of N-b of cation-cation (or anion-anion) pairs in the polyhedron, although the effect from the coordination shells beyond the neighboring ions is not negligible. (C) 2015 AIP Publishing LLC.
机译:通过全原子模型的分子动力学模拟检查了典型的离子液体1-乙基-3-甲基咪唑鎓硝酸盐(EMIM-NO3),以显示在玻璃化过程中笼形结构和/或键网络的特征。这种易碎的玻璃成型机。该系统显示出在其他易碎玻璃形成液中发现的两个特征温度(T-B(或T-c)和玻璃化转变温度T-g)下的动力学变化。 L. Ngai和J. Habasaki,J。Chem。物理141,114502(2014)]。随着温度降低,在对相关函数的第一个最小值g(r)(min)内,相邻阳离子对阴离子N-B的数量增加。在越过T-B(> T-g)时,系统体积和扩散系数都显示出温度依赖性的变化,并且通常在T-g处变化。玻璃化转变温度Tg的特征在于“键”总数NB的饱和,以及由N个粒子组成的体系的自由度相应降低,F = [(3N-6)-NB] 。其他离子对也具有类似的行为。因此,作为替代,玻璃化转变的动力学可以通过刚度渗透从概念上进行解释。在T-g出现饱和之前,键数在T-B附近显示出显着变化。该温度与阳离子周围的阴离子松散堆积的配位多面体的消失有关(反之亦然),这与每个配位多面体的多面体的几何自由度f(g)的丧失有关,其可由f定义(g)= [(3N(V)-6)-Nb]。在此,3N(v)是多面体的N-V个顶点的自由度,N-b是虚拟键的数目。多面体的填料的特征是笼子的软渗透,允许随着温度的降低而进一步变化。发现笼中中心离子位移的功率谱与多面体中阳离子-阳离子(或阴离子-阴离子)对的Nb波动相关,尽管配位壳对邻近离子的影响并不大微不足道。 (C)2015 AIP Publishing LLC。

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