三甲基铝双聚体和单体的气相离解-缔合平衡模拟计算

在B3LYP/6-31l++G(3df, 2pd)水平上全优化得到了三甲基铝双聚体(d-TMA)的C2h和C2v两种构型和单体的C3h结构. 着重用完全基组方法CBS-4M模拟计算了TMA气相平衡中各物种在1.01×105 Pa和300～550 K范围内的热力学函数值. 通过考察d-TMA三线态构型和异裂反应对系统熵值的影响, 准确计算了d-TMA离解反应的ΔrHm和ΔrSm. 以lnKd对1/T作图, 两者之间具有很好的线性关系: lnKd=−9624.4363/T+20.2303, 相关系数R2=1.0000, 与前人实验结果相当一致. 在此基础上提出了新的d-TMA气相离解-缔合反应机理.     

对-羟基苄叉丙二腈溶液在不同pH条件下吸收光谱的变化

在苄叉丙二腈衍生物系列中,N,N-二烷基氨基苄叉丙二腈及其类似化合物是研究和应用较多的一类。它们曾作为分子探针应用于高分子微环境特性和高分子聚合过程的研究。作为一种分子内的电荷转移络合物,它们在不同溶剂中的光谱行为也进行过研究,从而为进一步的开拓应用提供了重要依据。和前者相比,对-羟基苄叉丙二腈无论在基础研究或实际应用上都显得比较薄弱。正因如此,本工作合成了该化合物并对它进行了初步研     

Effect of combining rules for cubic equations of state on the prediction of double retrograde vaporization

In this work, the phenomenon of double retrograde vaporization (DRV) is simulated using the Peng–Robinson equation of state with the classical mixing rules and several combining rules for the cross-energy and cross-co-volume parameters. The binary interaction parameters are set equal to zero in all cases, i.e., the calculations are entirely predictive. An interesting conclusion is that the predictions using the classical combining rules (geometric mean rule for a_ij and arithmetic mean rule for b_ij) provide the best agreement with the experimental data for all the systems tested: methane + n-butane, methane + n-pentane, ethane + limonene, and ethane + linalool. Another interesting observation is that several combining rules for b_ij, other than the arithmetic mean rule, predict the existence of three phases in equilibrium in a very narrow temperature range close to the critical temperature of methane in the methane + n-pentane system, even though, literature data indicates that n-hexane is the first n-alkane to present partial liquid phase immiscibility with methane.     

Inter- and intramolecular potential for the N-formylglycinamide-water system. A comparison between theoretical modeling and empirical force fields

An intramolecular NEMO potential is presented for the N-formylglycinamide molecule together with an intermolecular potential for the N-formylglycinamide-water system. The intramolecular N-formylglycinamide potential can be used as a building block for the backbone of polypeptides and proteins. Two intramolecular minima have been obtained. One, denoted as C5, is stabilized by a hydrogen bonded five member ring, and the other, denoted as C7, corresponds to a seven membered ring. The interaction between one water molecule and the N-formylglycinamide system is also studied and compared with Hartree-Fock SCF calculations and with the results obtained for some of the more commonly used force fields. The agreement between the NEMO and SCF energies for the complexes is in general superior to that of the other force fields. In the C7 region the surfaces obtained from the intramolecular part of the commonly used force fields are too flat compared to the NEMO potential and the ab initio calculations. We further analyze the possibility of using a charge distribution obtained from one conformation to describe the charge distribution of other conformations. We have found that the use of polarizabilities and generic dipoles can model most of the changes in charge density due to the different geometry of the new conformations, but that one can expect additional errors in the interaction energies that are of the order of 1 kcal/mol.     

Reaction of β-aminopropionohydroxamic acid with aldehydes and ketones

β-Aminopropionohydroxamic acid reacts with aliphatic aldehydes or ketones to give 2-substituted 1-hydroxytetrahydropyrimidin-6-ones, while its reaction with aromatic carbonyl compounds leads to either the same products or Schiff's bases, which can exist in tautomeric equilibrium in solution. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 4, pp. 691–694, April, 1998.     

A potentiometric investigation of the hydrolysis of chromate (VI) ion in NaCl media to 175°C

The hydrolysis of chromate ion was studied potentiometrically in a concentration cell fitted with hydrogen electrodes by titrating basic NaCl–Na₂CrO₄ solutions with standardized HCl against a NaOH reference solution. The temperature was varied from 25 to 175°C at 25° intervals at the following ionic strengths (I): 0.1140, 0.2346, 0.5337, 0.9988, 2.940, and 5.239 (NaCl). Depending on the ionic strength, the molality of total chromium was varied from 0.001 to 0.100. The resulting titration curves could be resolved best in terms of three equilibria involving the formation of HCrO ₄ ^– (aq), Cr₂O^3– (aq), and CrO₃Cl^– (aq). The equilibrium quotients for all three reactions were fitted as a function of temperature and ionic strength, and the molal thermodynamic parameters that were computed from these relationships are tabulated at specific ionic strengths over the experimental temperature range.     

钠硼解石——水体系溶解和相平衡的研究(英)

Ulexite dissolution in water has been studied in the wide temperature range from 10℃ to 93℃ and two higher temperatures at 120 ℃ and 240 ℃. The analytical results showed that ulexite dissolved congruently from 10 ℃ to 35 ℃ and incongruently from 40 to 68 ℃. The solid component of ulexite, NaCaB₅O₆(OH)₆·5H₂O was dehydrated to form NaCaB₅O₆(OH)₆·H₂O from 50 to 68 ℃ and finally amorphous solid at 68 ℃. This amorphous solid converted into priceite at 71 ℃ and then converted completely to priceite at the boiling point(93℃) of the solution. At both 120 and 240 ℃, the dissolution of ulexite was an incongruent process. Above 120 ℃, ulexite became amorphous solid and then transformed into priceite. In addition to the solid to solid transformation, crystallization of priceite from the solution has also been observed. Based on our experimental results, mechanisms of dissolution, transformation, and crystallization of borate in ulexite-water system are discussed.     

Measurement of Diffusion in Zeolites—A Never Ending Challenge?

A review is given on the main problems associated with the determination and interpretation of molecular diffusion in zeolites. It is shown that the diffusivities may most decisively depend on the relevant space and time scales of observation, as well as on the physical state under which the measurements are carried out. Special emphasis is given to the microscopic techniques and their most recent evidence on the existence of transport resistances distributed over the intracrystalline space.