超临界正己烷甲醇溶液体系的 Monte Carlo 模拟──浓度对溶液构型影响的考察

用ＭｏｎｔｅＣａｒｌｏ分子模拟方法对正己烷－甲醇溶液体系处于临界状态时微观结构随浓度变化的情况进行了研究。模拟采用随机边界条件，得到了不同浓度条件下体系各基团的径向分布函数。结果表明，在溶液临界状态，正己烷分子有较强的聚集行为，随着溶液中甲醇浓度的变大，正己烷分子的聚集程度逐渐下降；甲醇分子周围正己烷分子的分布有一个最佳的浓度范围，在甲醇浓度为２２．５％时，配位数达到最大；超临界正己烷－甲醇溶液中甲醇分子的作用在不同浓度条件下具有不同的特点，当甲醇浓度较低时，甲醇分子之间有氢键的作用，随着甲醇浓度的提高，甲醇分子之间氢键的作用变得越来越弱，而且分子的取向变得越来越无序。     

甲醇在超临界环已烷中形成簇团的Monte Carlo初探

用Ｍｏｎｔｅ Ｃａｒｌｏ方法研究了甲醇－环己烷体系的微观结构随压力（密度）的变化情况，结果表明，在临界区域甲醇分子的聚集最为明显，形成的甲醇团簇尺寸最大，溶剂分子在甲醇周围的局部密度则在低于临界区或亚临界区较大。     

水-甲醇体系的Monte Carlo分子膜拟

本文应用Monte Carlo分子膜拟方法对水、甲醇水-甲醇的1:1混合物、甲醇无限稀释时的水溶液和水无限稀释时的甲醇溶液等五个体系进行了研究。采用TIP分子位能函数, 得到了上述体系的热力学性质、原子径向分布函数、分子氢键配位数分布。并以Monte Carlo分子模拟获得的结构函数与X射线衍射实验结果进行了比较。     

水-甲醇体系的Monte Carlo分子膜拟

本文应用Monte Carlo分子膜拟方法对水、甲醇水-甲醇的1:1混合物、甲醇无限稀释时的水溶液和水无限稀释时的甲醇溶液等五个体系进行了研究。采用TIP分子位能函数, 得到了上述体系的热力学性质、原子径向分布函数、分子氢键配位数分布。并以Monte Carlo分子模拟获得的结构函数与X射线衍射实验结果进行了比较。     

超临界正十二烷-醇溶液体系的Monte Carlo模拟

用ＭｏｎｔｅＣａｒｌｏ 方法研究了超临界正十二烷－醇溶液的分子质心Ｃ－ Ｃ、Ｃ－ Ｏ原子间的径向分布函数． 结果表明, 在临界压力下, 在临界温度附近改变温度时, 十二烷－十二烷分子质心Ｃ－ Ｃ原子间的径向分布函数变化不大, 即温度对十二烷分子间聚集的影响不明显． 在临界温度下, 当压力在临界压力附近变化时, 十二烷－十二烷分子质心Ｃ－ Ｃ原子间的径向分布函数发生了显著变化, 十二烷分子在临界压力以下聚集最强． 在临界状态下, 对于十二烷分别与甲醇、乙醇、正丙醇和异丁醇构成的溶液, 十二烷在异丁醇周围的聚集最强, 在乙醇周围的聚集次之, 在甲醇和正丙醇周围聚集较弱．     

亚临界和超临界二氧化碳-甲醇混合气相及液相区中甲醇核磁弛豫速率比较研究

用核磁共振氢谱测量了不同温度（293.15和308.15 K）及压力高达25 MPa下二氧化碳-甲醇混合气相（超临界）及液相区（亚临界）中甲醇（羟基及甲基）的纵向弛豫时间T_1,exp。本工作的目的是考察近临界区二氧化碳-甲醇混合物的压力、温度及组成对甲醇弛豫速率的影响,揭示混合物不同相区（气相及液相区）中自旋-晶格弛豫（SLR）过程的机理。此外,还对比研究了等温条件下超临界和亚临界混合气相及液相区中甲醇的SLR速率1/T_1,exp随混合物密度的变化规律。研究发现,在本工作所涉及的温度及压力区间,对于纯甲醇或液相区其SLR过程是以偶极-偶极（DD）作用机理为主导,而在气相区SLR过程则是以自旋-转动（SR）作用机理占优势,也即,超临界和亚临界二氧化碳-甲醇混合物的SLR过程在不同相区有不同的作用机理控制。由于甲醇的SLR弛豫速率1/T_1,exp是由甲醇分子间及分子内的DD作用和SR作用三部分共同决定的,所以研究超临界和亚临界二氧化碳-甲醇混合物的SLR弛豫速率随压力、浓度及温度的变化规律有助于提供更多该混合物不同相态区分子间相互作用的动态学信息。     

超临界正己烷—甲醇溶液体系的Monte Carlo模拟：浓度对溶液构型？…

用Ｍｏｎｔｅ Ｃａｒｌｏ分子模拟方法对正己烷－甲醇溶液体系处于临界状态时微观结构随浓度变化的情况进行了研究。模拟采用随机边界条件，得到了不同浓度条件下体系各基团的径向分布函数。结果表明，在溶液临界状态，正己烷分子有较强的聚集行为，随着溶液中甲醇浓度的变大，正己烷分子的聚集程度逐渐下降；甲醇分子周围正己烷分子的分布有一个最佳的浓度范围，在甲醇浓度为２２．５％时，配位数达到最大；超临界正己烷－甲醇溶液     

PNIPA和PDEA在水-甲醇混合溶剂中性质的研究

分别研究了聚N-异丙基丙烯酰胺（PNIPA）和聚N,N-二乙基丙烯酰胺（PDEA）在水-甲醇混合溶剂中的溶液性质.结果表明,在PDEA和PNIPA体系中均存在水和甲醇分子之间的复合.由于PDEA比PNIPA的亲脂性强,在水-甲醇混合溶剂中,水与甲醇分子形成的复合物对PDEA和PNIPA的溶剂化作用不同,导致随着体系中甲醇体积分数（φ）的增大,PNIPA体系的低临界溶解温度（TLCS）发生了再进入相转变,而PDEA体系的TLCS则逐渐升高.     

季铵盐从氰化物溶液中萃取金的研究:基于氢键结构的萃合物模型

通过 Ｆｏｕｒｉｅｒ变换红外光谱（ＦＴ－ＩＲ）,扩展Ｘ射线吸收精细结构（ＥＸＡＦＳ）,等离 子发射（ＩＣＰ）和同位素示踪等方法对氯化甲基三烷基铵（Ｎ２６３）－磷酸三丁酯（ＴＢＰ）－正十二 烷和Ｎ２６３－异辛醇－正十二烷从ＫＡｕ（ＣＮ）_２水溶液中萃取金的机理进行了深入的研究．应 用高分辨红外光谱证实负载有机相中ＣＮ伸缩振动吸收随萃金体系中助萃剂的不同而不 同,并将负载有机相中Ａｕ（ＣＮ）_２~－与助萃剂的相互作用归因于氢键机制,认为萃金体系中 的萃合物模型为基于氢键的超分子体系     

甲醇与不同碳链烷烃在超临界条件下溶液构型的分子模拟

用Montecarlo分子模拟方法,研究了甲醇与不同碳链的正构烷烃组成的不同浓度的溶液在超临界条件下的构型特征。模拟采用TIP势能函数,使用随机边界条件。模拟结果表明,在不同浓度的溶液中,甲醇周围烷烃介质的分布密度基本上相同,而对于不同介质中甲醇分子之间的积聚行为,不同浓度的溶液表现出不同的特点。当甲醇浓度较低时,甲醇在正戊烷、正己烷介质中形成团聚的程度最大,随着甲醇浓度的提高,甲醇分子之间的团聚趋弱。介质烷烃分子之间的积聚,基本上表现为:碳链越长,分子之间的团聚越加明显,而且,随着烷烃分子的浓度减小,这种趋势愈加明显。     

The influence of chain dynamics on the far-infrared spectrum of liquid methanol-water mixtures

Far-infrared-absorption spectroscopy has been used to study the low-frequency (相似文献   

Methanol in its own gravy. A PCM study for simulation of vibrational spectra

For studying both hydrogen bond and dipole-dipole interactions between methanol molecules (self-association) the geometry of clusters of increasing numbers of methanol molecules (n = 1,2,3) were optimized and also their vibrational frequencies were calculated with quantum chemical methods. Beside these B3LYP/6-311G** calculations, PCM calculations were also done for all systems with PCM at the same quantum chemical method and basis set, for considering the effect of the liquid continuum on the cluster properties. Comparing the results, the measured and calculated infrared spectra are in good accordance.     

Structure and dynamics of methanol in water: a quantum mechanical charge field molecular dynamics study

An ab initio quantum mechanical charge field molecular dynamics simulation was carried out for one methanol molecule in water to analyze the structure and dynamics of hydrophobic and hydrophilic groups. It is found that water molecules around the methyl group form a cage-like structure whereas the hydroxyl group acts as both hydrogen bond donor and acceptor, thus forming several hydrogen bonds with water molecules. The dynamic analyses correlate well with the structural data, evaluated by means of radial distribution functions, angular distribution functions, and coordination number distributions. The overall ligand mean residence time, τ identifies the methanol molecule as structure maker. The relative dynamics data of hydrogen bonds between hydroxyl of methanol and water molecules prove the existence of both strong and weak hydrogen bonds. The results obtained from the simulation are in excellent agreement with the experimental results for dilute solution of CH(3)OH in water. The overall hydration shell of methanol consists in average of 18 water molecules out of which three are hydrogen bonded.     

Intra- vs. intermolecular hydrogen bonding: dimers of alpha-hydroxyesters with methanol

Intermolecular hydrogen bonding competes with an intramolecular hydrogen bond when methanol binds to an alpha-hydroxyester. Disruption of the intramolecular OH...O=C contact in favour of a cooperative OH...OH...O=C sequence is evidenced by FTIR spectroscopy for the addition of methanol to the esters methyl glycolate, methyl lactate and methyl alpha-hydroxyisobutyrate in seeded supersonic jet expansions. Comparison of the OH stretching modes with quantum-chemical harmonic frequency calculations and 18O labelling of methanol unambiguously prove the insertion of methanol into the intramolecular hydrogen bond. This is in marked contrast to UV/IR hole burning studies of the homologous system methyl lactate: (+/-)-2-naphthyl-1-ethanol, where only addition complexes were found and the intramolecular hydrogen bond was conserved. This switch in hydrogen bond pattern from aliphatic to aromatic heterodimers is thought to reflect not only a kinetic propensity but also a thermodynamic preference for addition complexes when dispersion forces become more important in aromatic systems.     

UHV Studies of Methanol Decomposition on Mono‐ and Bimetallic CoPd Nanoparticles Supported on Thin Alumina Films

Bimetallic nanoparticles often turn out to be superior to the corresponding monometallic systems with respect to their catalytic properties. To study such effects for the methanol decomposition reaction, model catalysts were prepared by physical vapor deposition of Pd and Co under ultrahigh‐vacuum (UHV) conditions. Monometallic Pd and Co particles as well as CoPd core–shell particles were generated on an epitaxial alumina film grown on NiAl(110). The interaction with methanol is examined by temperature‐programmed desorption of methanol and carbon monoxide and by X‐ray photoelectron spectroscopy. The decomposition of methanol proceeds in two reaction pathways independent of the particle composition: complete dehydrogenation towards carbon monoxide and hydrogen, and C? O bond scission yielding carbon deposits. Pd is the most active material studied here. The relative importance of the two channels varies for the different particle systems: on Pd dehydrogenation is preferred, whereas the C? O bond cleavage is more pronounced on Co. The bimetallic clusters show a moderate performance for both pathways. Carbon deposition poisons the model catalysts by blocking the adsorption sites for methoxide, which is the first intermediate product during methanol decomposition. In particular on Co, large amounts of carbon deposits can also be caused by dissociation of the final product of the dehydrogenation pathway, carbon monoxide. A comparison with the results of methanol decomposition on Co, Pd, and CoPd catalysts in continuous‐flow reactors demonstrates that the findings of the present UHV study are relevant for catalytic performance under high‐pressure conditions.     

水、甲醇和乙醇液体微结构性质的Car-Parrinello 分子动力学模拟

采用Car-Parrinello 分子动力学(CPMD)方法分别研究了水、甲醇和乙醇的液体微结构性质.研究结果显示:在水、甲醇和乙醇三个体系中O…O径向分布函数曲线的第一个峰位置分别为0.278、0.276 和0.275nm; O…H径向分布函数曲线的第一个峰位置分别为0.178、0.176和0.177 nm.表明基团(氢原子、甲基、乙基)的差异对O…O第一个峰的位置影响很小.但基团的差异对径向分布函数峰高的影响却很显著,由水到乙醇第一个峰的高度逐渐变高.空间分布函数表明氧原子和氢原子在溶剂分子周围有取向地分布,这与径向分布函数所表现出尖锐的第一个峰相一致.氢键分布分析显示,水、甲醇和乙醇的平均氢键数分别为3.62、1.99 和1.87,表明水形成了网状氢键结构,而甲醇、乙醇形成链状氢键结构.     

Rotational Mechanism of Ammonium Ion in Water and Methanol?

Dynamics of ammonium and ammonia in solutions is closely related to the metabolism of ammoniac compounds, therefore plays an important role in various biological processes. NMR measurements indicated that the reorientation dynamics of NH₄⁺ is faster in its aqueous solution than in methanol, which deviates from the Stokes-Einstein-Debye rule since water has higher viscosity than methanol. To address this intriguing issue, we herein study the reorientation dynamics of ammonium ion in both solutions using numerical simulation and an extended cyclic Markov chain model. An evident decoupling between translation and rotation of methanol is observed in simulation, which results in the deviation of reorientation from the Stokes-Einstein-Debye rule. Slower hydrogen bond (HB) switchings of ammonium with methanol comparing to that with water, due to the steric effect of the methyl group, remarkably retards the jump rotation of ammonium. The observations herein provide useful insights into the dynamic behavior of ammonium in the heterogeneous environments including the protein surface or protein channels.     

Quantum-chemical study on reactions of isocyanates with methanol associates: VI. Quantum-chemical characterization of the relative reactivity of linear and cyclic methanol trimers in the addition to methyl isocyanate

Quantum-chemical study on the reaction of methyl isocyanate with cyclic methanol trimer at the B3LYP/6-311++G(df,p) level of theory showed that the process involves concerted asymmetric transition state in which the formation of new N-H bond outstrips the formation of new C-O bond. The reaction of methyl isocyanate with linear methanol trimer was found to be both kinetically and thermodynamically more favorable than with cyclic trimer.