高溶解性盐水体系热力学模型预测能力的比较研究Ⅰ：二元体系

用原始Pitzer模型、扩展的Pitzer模型、Pitzer-Simonson-Clegg模型、S-MSA模型和BET模型分别对LiCl-H2O,LiBr-H2O,CaCl2-H2O,Mg（NO3）2-H,O,MnCl2-H2O和Mn（NO3）2-H2O等六种不同体系的热力学性质进行描述,考察了各种模型的预测能力．结果表明原始Pitzer模型不能准确描述高浓电解质溶液的性质;扩展的Pitzer模型虽然能较准确地描述某些体系高浓度的热力学性质,但预测能力不足;Pitzer-Simonson-Clegg模型对高浓盐水体系热力学性质具有一定的预测能力,但拟合参数所用的最大浓度与溶解度相差很大时,外推饱和点的热力学性质则会出现较大偏差;S-MSA模型虽然可以将拟合参数的浓度范围扩大到饱和,但没有外推能力,而且需要溶液的密度数据,这限制了该模型的广泛应用：BET模型对这六种体系均体现出很强的预测能力,预测结果准确,且模型参数少,物理意义明确,该模型可用于熔盐水化物相变储能材料的设计．     

高溶解性盐水体系热力学模型预测能力的比较研究I: 二元体系

用原始Pitzer模型、扩展的Pitzer模型、Pitzer-Simonson-Clegg模型、S-MSA模型和BET模型分别对LiCl-H2O, LiBr-H2O, CaCl2-H2O, Mg(NO3)2-H2O, MnCl2-H2O和Mn(NO3)2-H2O等六种不同体系的热力学性质进行描述, 考察了各种模型的预测能力. 结果表明原始Pitzer模型不能准确描述高浓电解质溶液的性质; 扩展的Pitzer模型虽然能较准确地描述某些体系高浓度的热力学性质, 但预测能力不足; Pitzer-Simonson-Clegg模型对高浓盐水体系热力学性质具有一定的预测能力, 但拟合参数所用的最大浓度与溶解度相差很大时, 外推饱和点的热力学性质则会出现较大偏差; S-MSA模型虽然可以将拟合参数的浓度范围扩大到饱和, 但没有外推能力, 而且需要溶液的密度数据, 这限制了该模型的广泛应用; BET模型对这六种体系均体现出很强的预测能力, 预测结果准确, 且模型参数少, 物理意义明确, 该模型可用于熔盐水化物相变储能材料的设计.     

体系Mg(NO3)2-MgCl2-H2O作为相变储能材料的相图预测

应用修正的BET热力学模型对Mg(NO₃)₂-MgCl₂-H₂O体系在273～373 K的相图进行预测, 发现两个共晶点, 并通过实验对共晶点组成材料的吸热和放热行为进行测定, 发现三元共晶点Mg(NO₃)₂•6H₂O(45.6%)-Mg(NO₃)₂•2H₂O (29.6%)-MgCl₂•6H₂O(24.8%)储能效果较差, 而二元共晶点Mg(NO₃)₂•6H₂O(61.6%)-MgCl₂•6H₂O(38.4%)在熔点附近具有很好的储放热能力, 其相变热焓经差热分析为136.8 J•g^－1, 说明该材料可用作潜在的相变储能材料.     

聚合物溶液热力学模型的评述

预测聚合物溶液体系的气液平衡数据是热力学模型的一个重要内容.热力学模型大体可分3类,以过量吉布斯自由GF能表示的最为常用.本文选取基于GF的Flory-Huggins(FH)、UNIQUAC、UNIFAC和ENSIC 4种常用模型进行评述,认为FH模型出现较早,形式最简单;UNIQUAC模型发展较完善,应用范围较广,UNIFAC模型弥补了UNIQUAC模型参数缺乏的不足,应用最为;ENSIC模型具有较好的预测效果,但参数难以获得.     

二元及三元离子交换体系的统计热力学

本文用统计热力学方法对二元及三元离子交换体系进行了研究,得到了修正选择系数与交换剂组成关系的理论表达式,并得到二元交换体系的交换剂组分活度系数与组成的关系式,即Kielland公式。     

超临界二氧化碳与叔丁醇二元体系气液溶解度模型研究

采用固定体积可视观察法测量装置,在50～80℃温度范围内测定了CO2与叔丁醇于不同压力下的平衡数据.通过对高压状态下CO2在液相中的溶解度和叔丁醇在气相中的溶解度模型的研究,对亨利定律和Chrastil半经验溶解度方程进行了改进,提出了分别适合于高压状态下CO2与叔丁醇二元体系的相互溶解度模型.其中CO2在液相中的溶解度可用三次多项式模型关联,其形式为:Pco2=A+B1·xco2+B2·x2co2+b3·x3co2.叔丁醇在O2中的溶解度可用改进的Chrastil半经验溶解度方程进行模拟,其形式为C=ρk·exp(a/T)+b+c·ρm.结果表明,提出的气相溶解度方程和液相溶解度方程与实验数据有着较高的拟合相关系数和精度.     

热力学模型研究KNO3-K2SO4-H2O和KNO3-KCl-H2O体系溶解度

用Pitzer-Simonson-Clegg热力学模型(PSC模型),分别拟合KCl-H2O、K2SO4-H2O、KNO3-H2O体系以及KNO3-K2SO4-H2O和KNO3-KCl-H2O体系水活度和溶解度实验数据,得到二元参数和三元离子相互作用参数,并以此计算3个二元盐水体系溶解度相图,及2个三元盐水体系在不同温度下的溶解度,结果表明计算值与实验值一致。     

磷酸三丁酯与醇二元混合体系的热力学性质

用量热法测定了298.15 K时, 磷酸三丁酯(TBP)+甲醇/乙醇/正丁醇/正丙醇四个二元混合体系的超额混合焓及293.15 K和303.15 K时部分组成下的超额混合焓, 其值均在−0.3 − 0.3 kJ•mol−1之间, 且基本不受温度的影响. 用无热溶液模型计算了各体系的超额熵、超额Gibbs自由能及各组分的活度系数. 热力学分析表明, TBP+甲醇/乙醇/正丙醇二元体系能较好地符合无热溶液模型, 而TBP+正丁醇体系则不符合无热溶液模型.     

308.15K下NaCl-CaCl_2-H_2O体系热力学性质的等压研究

采用等压法研究了308.15K下NaCl-H2O、CaCl2-H2O和NaCl-CaCl2-H2O体系离子强度分别为0.5666～5.9265molkg-1、0.3943～5.5573molkg-1和0.6524～16.6631molkg-1的等压平衡浓度和水活度,计算了渗透系数及饱和蒸汽压,获得了该体系渗透系数和饱和蒸汽压随离子强度的变化规律.应用Pitzer离子相互作用模型,用实验数据用多元线性回归拟合了308.15K下该体系的NaCl和CaCl2的纯盐参数β(0)、β(1)、Cφ分别为0.3181、1.5346、-0.0014和0.07972、0.3067、0.00075,拟合标准偏差分别为0.00072、0.0049;混合离子作用参数θNa,Ca、ψNa,Ca,Cl分别为0.06821、-0.0076,拟合标准偏差为0.0063和0.0064.用Pitzer模型计算的渗透系数与实验结果吻合.本研究为含钠钙海卤水体系热力学模型建立提供了重要的热力学基础数据.     

萃取体系的热力学研究, 磷-32标记DBP分配法测定DBP-惰性溶剂二元体系的活度系数

本文采用我们提出的~(32)P标记DBP分配法测定DBP-惰性溶剂(苯、正己烷、四氯化碳、三氯甲烷、醋酸正戊酯和甲基环己酮等)二元体系中各种DBP浓度的活度系数。在多数情况下,DBP的活度系数可用下列公式表示 logf_2=aN_1~2和 losf_2=A/(1+By)~2 本文求得式中的常数和公式适用的范围,并根据实验的结果讨论了溶剂的影响。     

SCF MO LCGO studies on the hydration of ions: The systems H+H2O,Li+H2O,and Na+H2O

The energy surfaces of the systems LiOH ₂ ⁺ and NaOH ₂ ⁺ are studied for a number of different geometries within the SCF MO LCAO framework, using a gaussian basis set to approximate the wavefunction. In the minimum energy geometry of both systems the positive ion is bound to the oxygen atom of the water molecule. The computed binding energies and bond distances are: B ^SCF(LiOH ₂ ⁺ ) = 36.0 kcal/mole, d(LiO) = 3.57 a.u., and B ^SCF(NaOH ₂ ⁺ ) = 25.2 kcal/mole, d(NaO) = 4.23 a.u., resp. The results are compared with those of H₃O⁺ and discussed in view of ion-solvent interaction in aquous solutions.It is a pleasure to thank our technical staff for the careful preparation of the input for the programs and for its enthusiastic and skilful assistance in running the computer.     

Experimental Densities, Speeds of Sound, Isentropic Compressibilties and Shear Relaxation Times of CaSO4·2H2O + CaCl2 + H2O and CaSO4·2H2O + NaCl + H2O Systems at Temperatures 30 and 35 °C

Speeds of sound, u, have been measured as a function of concentration for the systems, CaSO₄·2H₂O +CaCl₂ + H₂O and CaSO₄·2H₂O + NaCl + H₂O, at temperatures of 30 and 35 °C. Derived parameters such as the isentropic compressibility, κ _S , and the shear relaxation time,τ,were calculated using the experimental speed of sound data in combination with viscosity values from our earlier work. Results have been compared with those of the CaCl₂+ H₂Oand NaCl + H₂O systems reported in literature,to examine the effect of adding CaSO₄·2H₂O(s).Values of κ _S for the system,CaSO₄·2H₂O + CaCl₂+H₂O,are smaller compared with those for the CaCl₂+ H₂O system.Values of τ are lower at lower concentrations and then cross over in a narrow concentration region.Values of κ _S for the system,CaSO₄·2H₂O+NaCl+H₂O, are also smaller when compared with those forthe NaCl +H₂O system.For this system the τ values are higher. These τ values reach a minimum at a certain concentration of NaCl in the solution and then increase with further increases in concentration.The influenceof solvent-separated and/or solvent-shared ion pairs plays a dominant role at higher concentrations for both systems.Results have been interpreted and discussed in terms of the expansion and contraction of the primary hydration shell of the ionic species present in the studied systems.     

Structures and rearrangement reactions of 4-aminophenol(H2O)1+ and 3-aminophenol(H2O)1+ clusters

In this paper the structures of 4-aminophenol(H2O)1+ and 3-aminophenol(H2O)1+ clusters are investigated in molecular beam experiments by different IR/UV-double resonance techniques as well as the mass analyzed threshold ionization spectroscopy yielding both inter- and intramolecular vibrations of the ionic and neutral species. Possible structures are extensively calculated at the level of density functional theory (DFT) or at the ab initio level of theory. From the experimental and theoretical investigations it can be concluded that in the case of 4-aminophenol(H2O)1 one O-H...O hydrogen-bonded structure exists in the neutral cluster but two structures containing either an O-H...O or a N-H...O hydrogen-bonded arrangement are observed in the spectra of the ionic species. This observation is a result of an intramolecular rearrangement reaction within the ion which can only take place if high excess energies are used. A reaction path via the CH bonds is calculated and explains the experimental observations. In the case of 3-aminophenol(H2O)1+ only one O-H...O bound structure is observed both in the neutral and ionic species. Ab initio and DFT calculations show that due to geometrical and energetical reasons a rearrangement cannot be observed in the 3-aminophenol(H2O)1+ cluster ion.     

Quantum mechanical calculations for the H2O + hnu --> O(1D) + H2 photodissociation process

Quantum mechanical wavepacket calculations for the photodissociation of water in the second absorption band are presented. Using O + H2 Jacobi coordinates, partial cross sections for the O(1D) + H2 channel are calculated for different initial rotational states. Conical intersection and Renner-Teller effects are included. The branching ratios for the four accessible dissociation channels at 121.6 nm are in good agreement with experiment (J. Chem. Phys. 1982, 77, 2432). The calculations predict significant rotational and vibrational excitation of the H2 fragments. Photodissociation of ortho and para water produces predominantly, but not exclusively, ortho and para H2 fragments, respectively.     

AX-BX2卤化物熔盐体系固溶体形成规律

用原子参数-模式识别方法研究了AX-BX2型卤化物熔盐体系形成固溶体的规律性，并应用人工神经网络方法对该体系形成的最大固溶度作定量计算，同时预报了LiC-NiCl2熔盐体系能形成以LiCl为基的广泛固溶体，其最大固溶度计算结果为21.5(mol)%NiCl2,与实验结果基本一致。     

Comparative XPS Study of Al2O3 and CeO2Sulfation in Reactions with SO2, SO2 + O2, SO2 + H2O,and SO2 + O2 + H2O

The interactions of Al₂O₃, CeO₂, Pt/Al₂O₃, and Pt/CeO₂ films with SO₂, SO₂ + H₂O, SO₂ + O₂, and SO₂ + O₂ + H₂O in the temperature range 300–673 K at the partial pressures of SO₂, O₂, and H₂O equal to 1.5 × 10², 1.5 × 10², and 3 × 10² Pa, respectively, were studied using X-ray photoelectron spectroscopy. The formation of surface sulfite at T 473 K (the S 2p _3/2 binding energy (E _b) is 167.5 eV) and surface sulfate at T 573 K (E _b = 169.2 eV) was observed in the reactions of Al₂O₃ and CeO₂ with SO₂. The formation of sulfates on the surface of CeO₂ occurred much more effectively than in the case of Al₂O₃, and it was accompanied by the reduction of Ce(IV) to Ce(III). The formation of aluminum and cerium sulfates and sulfites on model Pt/Al₂O₃ and Pt/CeO₂ catalysts occurred simultaneously with the formation of surface platinum sulfides (E _b of S 2p _3/2 is 162.2 eV). The effects of oxygen and water vapor on the nature and yield of sulfur-containing products were studied.     

Product spin-orbit state resolved dynamics of the H+H2O and H+D2O abstraction reactions

The product state-resolved dynamics of the reactions H+H(2)O/D(2)O-->OH/OD((2)Pi(Omega);v',N',f )+H(2)/HD have been explored at center-of-mass collision energies around 1.2, 1.4, and 2.5 eV. The experiments employ pulsed laser photolysis coupled with polarized Doppler-resolved laser induced fluorescence detection of the OH/OD radical products. The populations in the OH spin-orbit states at a collision energy of 1.2 eV have been determined for the H+H(2)O reaction, and for low rotational levels they are shown to deviate from the statistical limit. For the H+D(2)O reaction at the highest collision energy studied the OD((2)Pi(3/2),v'=0,N'=1,A') angular distributions show scattering over a wide range of angles with a preference towards the forward direction. The kinetic energy release distributions obtained at 2.5 eV also indicate that the HD coproducts are born with significantly more internal excitation than at 1.4 eV. The OD((2)Pi(3/2),v'=0,N'=1,A') angular and kinetic energy release distributions are almost identical to those of their spin-orbit excited OD((2)Pi(1/2),v'=0,N'=1,A') counterpart. The data are compared with previous experimental measurements at similar collision energies, and with the results of previously published quasiclassical trajectory and quantum mechanical calculations employing the most recently developed potential energy surface. Product OH/OD spin-orbit effects in the reaction are discussed with reference to simple models.     

Vibrational deactivation of HF(υ = 1) in the H2O + HF dimer: HF(υ = 1) + H2O(000) → HF(υ = 0) + H2O(001) + ΔE

The vibration-vibration energy transfer in the near-resonant collision HF(υ = 1) + H₂O(000) → HF(υ = 0) + H₂O(001) + ΔE = 205 cm^?1 has been investigated on the basis of the model of the nonrigid H₂O-HF dimer formation for temperatures not greatly higher than room temperature. The energy mismatch ΔE is considered to be removed by the slow translational motion of two molecules in the complex about their equilibrium separation. A strong negative temperature dependence of the energy exchange rate is shown between 300 and 500 K.