LiF-KCl熔盐溶液的Monte Carlo法计算机模拟研究 II: 熔体结构与物性的关系

本文用Monte Carlo法对互易盐系LiF-KCl熔盐溶液的局部结构作了计算机模拟。计算了该熔盐溶液的总势能和势能分布。在1200K模拟温度下, 该熔盐溶液中大部份离子组成各种形式的离子团。根据模拟的互易盐系熔盐溶液模型, 讨论了熔体局部结构和物性之间的关系。     

LiF-KCl熔盐溶液的Monte Carlo法计算机模拟研究——Ⅱ.熔体结构与物性的关系

本文用Monte Carlo法对互易盐系LiF-KCl熔盐溶液的局部结构作了计算机模拟。计算了该熔盐溶液的总势能和势能分布。在1200K模拟温度下,该熔盐溶液中大部分离子组成各种形式的离子团。根据模拟的互易盐系熔盐溶液模型,讨论了熔体局部结构和物性之间的关系。     

LiF-KCl熔盐溶液的Monte Carlo法计算机模拟研究——Ⅰ.径向分布函数和热力学性质

本文用Monte Carlo法对互易盐系LiF—KCl熔盐溶液的结构和性质进行了计算机模拟。计算了各离子的偏径向分布函数和摩尔容积、热焓、混合热等热力学性质。若干计算结果与实测值大体相符,计算表明:LiF—KCl熔盐混合后,Li~+,F~-离子间平均距离显著减小,熔体内自由体积作不均匀分布。本文还讨论了这一结构特点的成因和意义。     

ZnCl2熔盐的分子动力学模拟

近年来，若干作者根据几种粒子间函数，对ZnCl2熔盐结构做过分子动力学模拟［1－3］其出的Zn－Cl和Cl－Cl离子间的偏径向分布函数与中子衍射实测值符合较好，但Zn－Zn离子间距以及Zn－Zn间配位数计算值多偏高．鉴于Busing势函数在多价卤化物馆盐的分子动力学计算中应用效果较好[4],我们试用Busing势函数为基础对ZnCl2熔盐结构和能量做分子动力学计算．1研究方法计算所用粒子势为Busing势函数此处，Zi为离子的电行数（ZZn。＋＝2，Zcl－＝1），几；是离子有效半径，人为＊离子的“硬度”参数·据文献问，f二0．005071，尸zn。十二0．…     

芦丁的电喷雾离子阱质谱分析

研究了芦丁在电喷雾离子阱质谱(ESI-MS)下的主要特征碎片离子及其裂解规律。应用电喷雾离子阱质谱技术研究芦丁的结构和正、负离子扫描条件下芦丁的主要特征碎片离子及其裂解规律。芦丁在正、负离子模式下均可得到较好的质谱信息,在正离子模式下,容易与Na+形成[M+Na]+的准分子离子,并裂解形成碎片m/z 605,487,331,325,313,185等,在负离子模式下,形成[M-H]-的准分子离子,并进一步碎裂形成碎片m/z 301,283,257,255,229,227,211等。分别阐明了芦丁在正、负离子模式下的电喷雾质谱碎裂规律,并对主要特征碎片离子进行归属,为进一步芦丁的结构优化和修饰提供了有价值的依据。     

正负离子表面活性剂与两性表面活性剂的相互作用

本文研究正负离子表面活性剂与两性表面活性剂混合水溶液的表面性质, 以及两性表面活性剂对正负离子裘面活性剂溶解度的影响。结果表明: (1) 两性表面活性剂的加溶作用,有助于正负离子表面活性剂的溶解; (2) 加入两性表面活性剂的量适当, 混合溶液基本保持原正负离子表面活性剂的表面活性; (3) 正负离子表面活性剂与两性表面活性剂在表面层和胶团中分子间的相互作用比正负离子表面活性剂与非离子表面活性剂分子间的相互作用稍强HC-FC正负; 离子表面活性剂与两性表面活性剂混合体系在表面层中有可能形成双分子或多分子层结构。     

若干熔盐-液体金属溶液的量子化学研究

本文用量子化学方法研究了若干熔盐-液体金属溶液的微观结构.证明Li溶入LiF熔盐中形成Li_(n 1)~(n )或Li_(n 2)~(n )一类原子簇离子.LiF溶入液体Li后Li~ 离子空轨道参与金属键电子离域,离域能是Li和LiF熔体互相溶解的推动力.量子化学计算表明Mg_2~(2 )不如 Mg~ 和Mg_2~ 稳定.质谱实验亦证明 Mg~ 和Mg_2~ 的存在而不能发现Mg_2~(2 ).据此讨论了Mg在含Mg~(2 )熔盐中溶解的机理。     

Monte Carlo法计算机模拟研究冰晶石-氧化铝熔体结构

冰晶石-氧化铝熔液是由各类离子质点组成的相当复杂的混合物,研究此熔盐系的离子结构对探讨铝电解机理和氧化铝在冰晶石熔液中的溶解机理具有重要意义^[1],由于冰晶石-氧化铝的熔点高和腐蚀严重,一些衍射技术难以用于此熔盐系液态微观结构性质的研究。     

NaCl-NaBr系熔盐溶液的分子动力学研究

近年来，用计算机模拟馆公的结构和性质的研究已有较大进展[1，2]．但研究工作多集中在有阴离子相同、阳离子不同的盐组成的“同阴离子系”（commonanionsystems），而对由阳离子相同、阴离子不同的盐组成的“同阳离子系”（commoncationsystems）熔盐溶液则甚少研究．鉴于自然界和生产中同阳离子系也不乏实例，建立同阳离子系熔盐溶液的理论屯有必要．为止匕我们先选择NaCI－NaBr系熔盐溶液（同阳离子系的一个最简单的典型）为对象，开展分子动力学方法计算机模拟研究．1模型和计算方法采用标准文献中的计算模拟和方法，离子间劳用Fumi-…     

MgCl2在LiCl-KCl熔盐中的电化学特性

研究了温度范围在723-908 K的LiCl-KCl 熔盐体系中MgCl₂的电化学行为和热力学性质. 循环伏安和方波伏安法研究表明镁离子的电化学还原过程为包含了两个电子转移的一步反应. 利用Berzins 和Delahay 方程计算了不同温度下的镁离子的扩散系数, 并通过Arrhenius 公式计算了镁离子在LiCl-KCl 熔盐体系中的扩散活化能. 采用开路计时电位法得到了不同温度下的Mg(II)/Mg(0)体系的平衡电位, 并结合电动势法计算了在LiCl-KCl 熔盐体系中Mg(II)/Mg(0)体系的标准形式电位. 根据不同温度下的标准形式电位, 计算得到了MgCl₂在LiCl-KCl 熔盐体系中的熵变和焓变以及不同温度下的活度系数.     

Electronic absorption spectra of the cations and anions formed from pyrrole analogs of the chalcones

The electronic absorption spectra of 29 pyrrole analogs of the chalcones have been studied in solutions of strong acids and alkalies, in which the corresponding cations and anions are formed. It has been shown by means of the IR spectra that the protonation of the pyrrole chalcones takes place at the carbonyl group. Considerations are given of the structure of the organic cations and anions studied and of the characteristic features in the change in their coloration as a function of their chemical structure. Satisfactory correlations have been found between the shift of the absorption frequency of the long-wave band which takes place at the transition from a neutral solution (molecules) to an acid solution (cations) or to an alkaline solution (anions) and Hammett's o constants. Three 3-(4-halophenyl)-1-(2-pyrryl)propenones not previously reported in the literature have been synthesized.     

Electronic absorption spectra of the cations and anions formed from pyrrole analogs of the chalcones

The electronic absorption spectra of 29 pyrrole analogs of the chalcones have been studied in solutions of strong acids and alkalies, in which the corresponding cations and anions are formed. It has been shown by means of the IR spectra that the protonation of the pyrrole chalcones takes place at the carbonyl group. Considerations are given of the structure of the organic cations and anions studied and of the characteristic features in the change in their coloration as a function of their chemical structure. Satisfactory correlations have been found between the shift of the absorption frequency of the long-wave band which takes place at the transition from a neutral solution (molecules) to an acid solution (cations) or to an alkaline solution (anions) and Hammett's o constants. Three 3-(4-halophenyl)-1-(2-pyrryl)propenones not previously reported in the literature have been synthesized.     

Impact of anisotropy on the structure and dynamics of ionic liquids: a computational study of 1-butyl-3-methyl-imidazolium trifluoroacetate

The complex ionic network of 1-butyl-3-methyl-imidazolium trifluoroacetate was simulated by means of the molecular dynamics methods over a time period of 100 ns. The influence of the anisotropy of the shape and charge distribution of both the cations and the anions on the local (molecular) and global (collective) structure and dynamics is analyzed. The distance-dependent g coefficients of the orientational probability function g(r,Omega) were found to be an excellent way to interpret local structure. Thereby, the combination and interrelation of individual g coefficients elucidate the mutual orientation. Dynamics at the molecular level is characterized by the time correlation function of the center-of-mass corrected molecular dipole moment mucm. Upon uniting the set of molecular dipoles to a single collective rotational dipole moment, MD, dynamics on a global level is studied. Decomposing into subsets of cations and anions respective self terms as well as the prominent cross term can be extracted. This decomposition also enables a detailed peak assignment in dielectric spectra.     

Anion-promoted cation motion and conduction in zeolites

The motion of sodium cations in sodalite and cancrinite has been investigated by force field calculations, solid-state NMR, and impedance spectroscopy. Special emphasis is dedicated to the influence of anions on sodium mobilities. Local cation motion is promoted when they interact with anions. However, not all systems with high local mobilities exhibit good ion conductivities, as cooperativity of the motion appears to be an important factor, as well. The activation barrier for local sodium motion (calculations) and long-range transport (dc conductivities) is lowered in sodalite when halogenide anions, Cl(-), Br(-), or I(-), are present. The activation barriers increase with increasing size of the anion and decreasing coordination in the transition state. On the basis of (23)Na solid-state NMR data, all the sodium ions in the dense sodalite structure are rather rigid up to 470 K. All the cations in chromate sodalite, and Na(+) in the small cancrinite epsilon-cages without anion interactions, show a restricted local motion at higher temperatures. There is a selective high local motion of Na(+) in the neighborhood of chromate anions in the more open channel system of cancrinite. These results suggest that sodium migration can be enhanced, at least locally, in open channel systems by anion interactions. A dynamics coupling between anion reorientation and cation mobility was not observed.     

Ab initio molecular dynamics of liquid 1,3-dimethylimidazolium chloride

Density-functional-based Car-Parrinello molecular dynamics (CPMD) simulations have been performed for the ionic liquid 1,3-dimethylimidazolium chloride, [dmim]Cl, at 438 K. The local structure of the liquid is described in terms of various partial radial distribution functions and anisotropic spatial distributions, which reveal a significant extent of hydrogen bonding. The cation-anion distribution simulated with the BP86 functional is in qualitative agreement with the structural model derived from neutron diffraction data for the liquid, whereas the theoretical cation-cation distribution shows less satisfactory accord. Population analyses indicate noticeable charge transfer from anions to cations, and specific CH...Cl hydrogen bonds are characterized in terms of donor-acceptor interactions between lone pairs on Cl and antibonding sigma(CH) orbitals.     

Molecular Dynamics Simulation of Ion Sputtering of a Sodium Chloride Solution

The sputtering of an aqueous solution of sodium chloride with a concentration of 0.5 mol/L under bombardment by 1–20 positive ions with initial energies of 50–500 eV has been simulated by a molecular dynamics method. It has been found that the transfer of solute cations and anions to a gas phase requires a threshold energy of bombardment. It has been shown that the solute components occurred in the gas phase both as hydrated ions and in the form of ion pairs in the composition of water clusters. As the energy input into the cell reached ~0.33 eV/particle, the clusters of five or more water molecules were predominantly sputtered.     

Identification of 1,3-dialkylimidazolium salt supramolecular aggregates in solution

The nature of the interactions between 1,3-dialkylimidazolium cations and noncoordinating anions such as tetrafluoroborate, hexafluorophosphate, and tetraphenylborate has been studied in the solid state by X-ray diffraction analysis and in solution by (1)H NMR spectroscopy, conductivity, and microcalorimetry. In the solid state, these compounds show an extended network of hydrogen-bonded cations and anions in which one cation is surrounded by at least three anions and one anion is surrounded by at least three imidazolium cations. In the pure form, imidazolium salts are better described as polymeric supramolecules of the type {[(DAI)(3)(X)](2+)[(DAI)(X)(3)](2-)}(n) (where DAI is the dialkylimidazolium cation and X is the anion) formed through hydrogen bonds of the imidazolium cation with the anion. In solution, this supramolecular structural organization is maintained to a great extent, at least in solvents of low dielectric constant, indicating that mixtures of imidazolium ionic liquids with other molecules can be considered as nanostructured materials. This model is very useful for the rationalization of the majority of the unusual behavior of the ionic liquids.     

The influence of hydrogen bonding on the physical properties of ionic liquids

Potential applications of ionic liquids depend on the properties of this class of liquid material. To a large extent the structure and properties of these Coulomb systems are determined by the intermolecular interactions among anions and cations. In particular the subtle balance between Coulomb forces, hydrogen bonds and dispersion forces is of great importance for the understanding of ionic liquids. The purpose of the present paper is to answer three questions: Do hydrogen bonds exist in these Coulomb fluids? To what extent do hydrogen bonds contribute to the overall interaction between anions and cations? And finally, are hydrogen bonds important for the physical properties of ionic liquids? All these questions are addressed by using a suitable combination of experimental and theoretical methods including newly synthesized imidazolium-based ionic liquids, far infrared spectroscopy, terahertz spectroscopy, DFT calculations, differential scanning calorimetry (DSC), viscometry and quartz-crystal-microbalance measurements. The key statement is that although ionic liquids consist solely of anions and cations and Coulomb forces are the dominating interaction, local and directional interaction such as hydrogen bonding has significant influence on the structure and properties of ionic liquids. This is demonstrated for the case of melting points, viscosities and enthalpies of vaporization. As a consequence, a variety of important properties can be tuned towards a larger working temperature range, finally expanding the range of potential applications.     

Electrostatic interaction of ion-penetrable membranes. Effects of ionic solubility

An analytic, approximate expression for the electrostatic interaction between two membranes immersed in an electrolyte solution is derived on the basis of a simple membrane model. This model assumes that the membrane has a surface layer in which charged groups are uniformly distributed and that electrolyte ions can penetrate into the surface layer. The partition coefficients of cations and anions between the solution and the surface layer, which are related to their solubilities in the surface layer, may be different from unity.The electrostatic interaction depends on the ionic partition coefficients between the solution and the surface layer, and the relative permittivity of the surface layer, as well as on the membrane-fixed charges, the electrolyte concentration in the solution, and the surface layer thickness. It is shown, in particular, that even where the charge layer has no fixed charges, the electrostatic interaction force can be produced if the solubilities of cations and anions are different in the surface layer.     

Hydrogen bonding mediated ion pairs of some aprotic ionic liquids and their structural transition in aqueous solution

Ion pair speciation of ionic liquids(ILs) has an important effect on the physical and chemical properties of ILs and recognition of the structure of ion pairs in solution is essential. It has been reported that ion pairs of some ILs can be formed by hydrogen bonding interactions between cations and anions of them. Considering the fact that far-IR(FIR) spectroscopy is a powerful tool in indicating the intermolecular and intramolecular hydrogen bonding, in this work, this spectroscopic technique has been combined with molecular dynamic(MD) simulation and nuclear magnetic resonance hydrogen spectroscopy(~1H NMR) to investigate ion pairs of aprotic ILs [Bmim][NO_3], [BuPy][NO_3], [Pyr_(14)][NO_3], [PP_(14)][NO_3] and [Bu-choline][NO_3] in aqueous IL mixtures. The FIR spectra have been assigned with the aid of density functional theory(DFT) calculations, and the results are used to understand the effect of cationic nature on the structure of ion pairs. It is found that contact ion pairs formed in the neat aprotic ILs by hydrogen bonding interactions between cation and anion, were still maintained in aqueous solutions up to high water mole fraction(say 0.80 for [BuPy][NO3]). When water content was increased to a critical mole fraction of water(say 0.83 for [BuPy][NO3]), the contact ion pairs could be transformed into solvent-separated ion pairs due to the formation of the hydrogen bonding between ions and water. With the further dilution of the aqueous ILs solution, the solvent-separated ion pairs was finally turned into free cations and free anions(fully hydrated cations or anions). The concentrations of the ILs at which the contact ion pairs were transformed into solvent-separated ion pairs and solvent-separated ion pairs were transformed into free ions(fully hydrated ion) were dependent on the cationic structures. These information provides direct spectral evidence for ion pair structures of the aprotic ILs in aqueous solution. MD simulation and ~1H NMR results support the conclusion drawn from FIR spectra investigations.