聚N,N-二乙基丙烯酰胺低聚物水溶液的分子动力学研究

对50个单元构成的聚N,N-二乙基丙烯酰胺(PDEA)低聚物的水溶液体系进行了分子动力学的研究,分别模拟了300 K时的伸展链、310 K时的伸展链以及紧缩链与水构成的体系,对溶液中PDEA周围溶剂水分子的分布情况以及水分子形成氢键的情况进行了统计,结果表明在PDEA周围的水产生了比本体水更有序的结构,形成了更多的氢键,这种有序结构维持到第二水合层甚至更远.发生相分离后,PDEA与水分子形成的氢键大部分未被破坏,水合层中每个水分子形成的氢键数也没有明显变化,但水合层(形成有序结构的水分子)内水分子数目的减少使得总的氢键数目减少,从而造成体系能量增加及熵增加.同时还研究了聚合物及水分子的自扩散系数,表明PDEA影响周围水分子结构的同时,对水的动力学性质也产生了很大影响.     

液态水的分子动力学模拟

用分子动力学(MD)模拟方法在150～376K的温度范围内对液态水的微正则系综进行了研究.考察了液态水的结构及其性质.模拟采用了由从头算得出的柔性水-水相互作用势MCYL.对时间和空间的平均得出了液态中水分子几何构型及温度改变所引起的液态水结构变化.对径向分布函数g_(OH),goo,g_(HH)及配位数的分析表明,在所考察的温度范围内,每个水分子与相邻分子形成的氢键数为2～3,水分子在参与的2个氢键中同时作为接受体.结合对振动谱的研究表明在低温时液态水形成的网络结构可能随温度的升高而形成小的簇结构.     

液态水几何构型的分子动力学模拟

利用ＭＣＹＬ势对液态水进行分子动力学模拟，以探求近程和远程相互作用及液体的有序结构对水分子几何构型的影响，并确定对液态中水分子几何构型起作用的主要范围。模拟给出的液态水中原子对径向分布函数和水分子键长键角的变化与实验值能较好地符合。研究结果表明，液态水分子几何构型除与氢键的形成有关外，还与液体的近程有序结构有很大关系。键长的变化对这种近程有序结构虽不敏感，但键角的变化则对此非常灵敏。液态中第二水合     

NH4+( (H2O)n(n＝1～9)的量子化学和ABEEM/MM的理论研究

运用量子化学和ABEEM/MM浮动电荷分子力场, 构建描述铵离子-水体系相互作用的精密势能函数, 对 - (H₂O)_n (n＝1～9)簇合物的结构和稳定性等性质进行了研究. 对团簇的结合能和电荷布居分析发现, 当n≤4时, 随着水分子数目的增加, 与水分子间尽可能多地形成线型氢键, 直至水分子在 周围形成完整的第一水合层|当n≥5时, 簇合物以 为中心, 通过氢键网络形成的环状和笼状结构为最稳定. 与第一水合层水分子的相互作用强于水分子之间的相互作用. 结果表明, ABEEM/MM方法的结果与量子化学方法得到的结果有很好的一致性.     

液态水的分子动力学模拟

用分子动力学(MD)模拟方法在150~376K的温度范围内对液态水的微正则系统进行了研究。考察了液态水的结构及其性质。模拟采用了由从头算得出的柔性水-水相互作用势MCYL。对时间和空间的平均得出了液态中水分子几何构型及温度改变所引起的液态水结构变化。对径向分布函数gOH, gOO, gHH及配位数的分析表明, 在所考察的温度范围内, 每个水分子与相邻分子形成的氢键数为2~3, 水分子在参与的2个氢键中同时作为授受体。结合对振动谱的研究表明在低温时液态水形成的网络结构可能随温度的升高而形成小的簇结构。     

离子对水结构的影响

液态水中广泛存在的氢键网络使其作为一种结构性很强的液体在自然界中发挥着独一无二的作用。电解质溶于水中后,以水合离子形式存在,离子附近强大的电场使水合层中的偶极水分子发生重排,这些水分子的结构与本体水的结构存在差异。一个多世纪以来,科学家做了大量关于离子对水结构影响的研究。本文从静态谱学和溶剂动力学两方面综述了离子对水结构影响的研究进展,概括了水中氢键的研究情况,并就离子对水结构影响在生物化学方向的重大意义-Hofmeister效应作了解释。     

水化镁基蒙脱石的分子动力学模拟

利用分子动力学(MD)模拟了300 K时镁基蒙脱石(粘土)层间水和镁离子的结构和动力学性质.模拟结果显示水在粘土层间分为二层,只有一小部分水被粘土表面吸附,与粘土结构中的羟基形成氢键,不同分布位置的水处于动态平衡.层间水分子氢键配位数比普通水少24%左右,水在粘土中自扩散系数D＝5.355×10^-10 m²·s^-1,约为主体相水的1/4.镁离子在粘土层间形成一层,其与水分子配位数约为6.进一步讨论了温度对粘土层中水的结构和动力学性质的影响.随着温度升高,水层的局部密度ρ(z)降低,水在XY方向的扩散系数不断增大.当温度达到600 K后,层间水分子间的氢键断裂,与超临界状态下水的结构相似,层间水的扩散系数达最大值,温度进一步升至700 K时,其值基本无变化.     

RbCl和CsCl水溶液结构的X射线散射及经验势结构精修模拟

采用X射线散射法研究了RbCl和CsCl水溶液的结构,利用基于经验势的结构精修(EPSR)方法获得了溶液中的水合Cl^-、Rb⁺、Cs⁺、离子缔合及本体水的对径向分布函数、配位数分布及空间密度分布(3D结构)等结构信息。在水溶液中,Cl^-具有相对稳定的6水合结构,其水合距离为0.321 nm,外加阳离子对其水合作用的影响不明显。7.3 ± 1.4个水分子与Rb⁺水合,其特征水合距离为0.297 nm,8.4 ± 1.6个水分子与Cs⁺水合其水合距离为0.312 nm。Cs⁺不具有第二水合层,而Rb⁺表现出了更强的水合能力,具有较明显的第二水合层。Cl^-、Rb⁺及Cs⁺常被认为是“结构破坏”型离子。从微观角度来看这种所谓的“结构破坏”主要体现在破坏了本体水分子的第二水合层保持四面体构型的趋势。RbCl和CsCl水溶液中部分存在着Rb-Cl和Cs-Cl直接接触离子对,在1.0 mol·dm^-3的溶液中Rb-Cl及Cs-Cl的特征距离分别为0.324和0.336 nm,溶剂分割离子对的距离则都在0.6 nm左右。相对于Cs⁺,Rb⁺与Cl^-离子之间表现出了更强的缔合能力。     

二水合甘氨酸两性离子复合体的结构和性能的理论研究

采用理论计算方法B3LYP, 在6-31++G**基组水平研究使甘氨酸质子化所需的最少水分子数目, 然后讨论水合两性离子复合体的结构和性能, 进而计算了二水合甘氨酸中性分子复合体(2W-GN)到二水合甘氨酸两性离子复合体(2W-GZ)的过渡态, 得到如下结论: (1)两个水分子可以使甘氨酸质子化, 能够形成稳定的二水合两性离子复合体. (2)甘氨酸与水分子之间通过氢键相互作用, 结合能较大, 复合体稳定; 在二水合甘氨酸复合体中, 水合甘氨酸中性分子比水合甘氨酸两性离子稳定. (3)由2W-GN到2W-GZ过程的反应活化能和氢键键能相近.     

二氟尼柳/水滑石插层组装结构、氢键及水合特性的分子动力学模拟

采用分子动力学方法模拟二氟尼柳插层水滑石(DIF/LDHs)的超分子结构, 研究复合材料主客体间形成的氢键以及水合膨胀特性.结果表明, 当水分子总数与DIF分子总数之比Nw≤3时, 层间距dc保持基本恒定, 约1.80 nm; 当Nw≥4时, 层间距逐渐增大, 且符合dc=1.2611Nw+13.63线性方程. 随着水分子个数增加, 水合能驻UH逐渐增大. 当Nw≤16时, 由于⊿UH<-41.84 kJ·mol-1, LDHs-DIF可以持续吸收水, 从而使材料层间距不断膨胀. 但当Nw≥24时, ⊿UH>-41.84 kJ·mol-1, 此时LDHs-DIF层间不能再进一步水合, 因此LDHs-DIF在水环境中膨胀具有一定的限度. 水滑石层间存在复杂的氢键网络. DIF/LDHs水合过程中, 水分子首先同步与层板和阴离子构成氢键; 当阴离子趋于饱和后, 水分子继续与层板形成氢键, 并逐步发生L-W型氢键取代L-A型氢键, 驱使阴离子向层间中央移动, 与层板发生隔离; 最后水分子在水滑石羟基表面形成有序结构化水层.     

Measurements of Rayleigh scattering and relativistic calculations of incoherent scattering functions

Recent measurements of Rayleigh scattering employing neutron capture γ-rays are presented. Experimental conditions are achieved such that the Rayleigh contribution is dominant and much larger than the other competing coherent processes. A detailed comparison with the modified relativistic form factor (MRFF) approximation is made and it is concluded that the latter overestimates the cross-section by 3–4%. New calculations of S, the incoherent scattering function, are presented in the relativistic treatment of Ribberfors and Berggren, using multiconfiguration Dirac–Fock relativistic wavefunctions. Tables of S, for Z=1–110, are shown on a momentum transfer mesh identical to previous non-relativistic calculations. S has been calculated at a representative angle θ=60° and energies compatible with the presentation mesh. For other scattering angles, the values presented in the tables are accurate to within 1–2% for momentum transfers larger than 0.1 Å⁻¹. In the region below 0.1 Å⁻¹ the accuracy worsens with decreasing momentum transfer, reaching 6% at 0.01 Å⁻¹ and 10% at 0.005 Å⁻¹. The same multiconfiguration wave functions were used to evaluate new MRFFs. The new elastic scattering cross sections differ by 3–6% compared with calculations based on single configuration wave functions.     

Characterization of polymer materials by scattering techniques,with applications to block copolymers

The application of six techniques—static and dynamic light scattering, small-angle neutron and X-ray scattering, neutron and X-ray reflectivity—to the characterization of polymer materials is summarized. Emphasis is placed on the similarities and differences among the various techniques, and on recent advances in experimental practice. Twelve examples from the recent literature are described, most of which concern block copolymers. A brief introduction to block copolymer properties is also provided.     

Study on the resonance Rayleigh scattering spectra and resonance non-linear spectra of congo red-amikacin system and its analytical application

The interaction between congo red (CR) and amikacin (AMK) was studied by resonance Rayleigh scattering (RRS), frequency doubling scattering (FDS) and second-order scattering (SOS) combining with absorption spectrum. In a weak acidic medium, CR combined with AMK to form an ion association complex with the composition ratio of 1∶1 by electrostatic interaction, hydrophobicity and charge transferring effect. As a result, the new spectra of RRS, FDS, and SOS appeared and their intensities were enhanced greatly. The maximum wavelengths of RRS, FDS and SOS were located at 563 nm, 475 nm and 940 nm, and the scattering intensities were proportional to the concentration of AMK. These three methods have very high sensitivities, and the detection limits were 4.0 ng·mL?1 for RRS, 3.6 ng·mL?1 for FDS and 1.9 ng·mL?1 for SOS, respectively. At the same time, the methods have better selectivity. A new method for the determination of trace amounts of AMK with congo red by resonance scattering technique has been developed. The recovery for the determination of AMK in blood serum and urine sample was between 95.5% and 105.5%. In this study, the properties, such as enthalpy of formation, charge distribution and mean polarizability, were calculated by AM1 quantum chemistry method. In addition, the reaction mechanism and the reasons for the enhancement of scattering spectra were discussed.     

大肠杆菌的共振散射光谱研究

研究了大肠杆菌的共振散射光谱.它在470nm、510nm和730nm产生三个瑞利散射峰.当激发波长为470nm(6.38×1014Hz)时,大肠杆菌溶液在470nm(6.38×1014Hz)和940nm(1/2×6.38×1014Hz)分别产生一个瑞利散射峰和一个1/2分频散射峰;当激发波长为510nm(5.88×1014Hz)时,在510nm产生一个共振散射峰;当激发波长为730nm(4.11×1014Hz)时在365nm(2×4.11×1014Hz)和730nm(4.11×1014Hz)分别产生一个2倍频散射峰和一个共振散射峰.分频散射和倍频散峰与共振散射峰具有相似的散射行为.大肠杆菌的浓度在0.074～38×108个/mL范围内与共振光散射强度I470nm、I510nm、I730nm成良好线性关系.     

Inhomogeneity control in polymer gels

Inhomogeneities, that is, nonrelaxing frozen concentration fluctuations, are inevitably present in polymer gels because they are introduced during the crosslinking of the constituent polymer chains in a solvent. Therefore, inhomogeneities increase as the number of crosslinks increases in a gel. The ionization of polymer gels is one of the methods used to suppress inhomogeneities. However, because crosslinking also means a freezing‐in of the conformation and topology of polymer chains in a solvent according to the chemistry of crosslinking, inhomogeneity control is quite sophisticated. In this article, we discuss the relationship between the inhomogeneities and the molecular/environmental parameters of polymer gels, such as the polymer concentration, the degree of crosslinking, the degree of ionization, and the interaction parameter, by considering the memory effect of gels. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 617–628, 2005     

Frequency-dependence of the polarizability anisotropy of CO2 revisited

We present extended determinations of the polarizability anisotropy κ(ω) of CO₂ at 514.5 and 488.0 nm by means of measuring the depolarization ratio ρ(ω) of linearly polarized laser light. Taking into account the hitherto reported data on ρ(ω) as well as experimental data on the mean polarizability (ω) and additional information derived from Kerr-effect measurements, we obtain a value of the static polarizability anisotropy of CO₂ of κ(0)=15.2(1.6) au. The large uncertainty of ≈10% results from the fact that all available experimental information is used to obtain an estimate of the static polarizability ansiotropy of CO₂. This zero-frequency value, which includes the vibrational part of the static anisotropy, is in reasonable agreement with hitherto reported experimental data and in good accordance with new ab initio calculations.     

Attractive interactions in critical scattering from non-ionic micelles

We have studied the temperature-dependent critical scattering of both light and neutrons from aqueous solutions ofn-octyl pentaoxyethylene glycol monoether (C₈E₅). We show that the assumption of a short-ranged temperature-dependent attractive pair potential between approximately spherical micelles of constant size permits a quantitative analysis of the neutron scattering data. The analysis, which is undertaken using current liquid-state theory and is in analytic form, contains only one free parameter, the depth of the attractive potential. We find that a potential with a range of only a fraction of a nm is sufficient to generate spatial correlations over tens of nm as the attractive potential deepens on approaching the critical temperature. The analysis also provides a semi-quantitative understanding of the light scattering data as a function of concentration and temperature, and leads to a qualitative prediction of the form of the phase diagram. Numerical values obtained are consistent with the hypothesis that the primary effect of raising the temperature is to lower the degree of structure of water near the micelle surface, allowing increased van der Waals attraction due to closer contact.     

A systematic treatment of three-dimensional quantum mechanical reaction coordinates

Summary The rigorous, collinear, canonical point transformation method with hyper-hyperbolic coordinates is extended to the infinite central mass problem in three dimensions. The initial transformation performed is (x_A, y _A, z _A, x _C, y _C, z _C) (, , , r, R, ), where (, , ) are the Euler angles; r and R are the AB and BC interatomic distances, respectively, and is the angle between r and R. A second transformation is then performed to (, , , , , ), where is the reaction coordinate mimicking the reaction path, and is the vibrational coordinate of the diatom. The transformed spaces are all one-to-one mappings from the original spaces, and thus do not have any three-to-one regions. The transformed momenta and Hamiltonians are derived, and are Hermitian in their respective transformed spaces.