用新的路径定位指数和神经网络研究多溴联苯醚理化性质

基于溴取代基及共轭母体的结构特征,定义一种新的路径定位指数mP,并计算了209种多溴联苯醚分子的电性拓扑状态指数E9和电性距离矢量M26,这3个指数对有机污染物呈现出良好的结构选择性。采用多元回归方法对多溴联苯醚(PBDEs)的色谱保留时间(tR)、正辛醇/空气分配系数(lgKOA)、超冷流体蒸气压(lgPL)及其毒性等性质与分子结构指数进行关联,建立的4个预测模型的相关系数分别达到0.991、0.997、0.998和0.904,标准偏差分别为0.031、0.104、0.100和0.358。将3个指数作为BP神经网络的输入层神经元,采用不同的网络体系结构,获得了令人满意的预测理化性质的神经网络模型,所得结果明显优于多元回归方法,结果显示多溴联苯醚的理化性质与0P、E9和M26具有良好的非线性关系。     

多溴联苯醚理化性质的定量构效关系

为研究多溴联苯醚（PBDEs）理化性质,提出其分子中顶点原子（基团）特征值（δ_i）新的计算方法,并在修正的距离矩阵基础上构建了拓扑距离特征定位指数（T）;采用文献程序软件和Gaussian 03程序软件分别计算,得到其分子电性距离矢量（M_t）和多种量子化学参数。用最佳变量子集回归方法建立了相关参数与PBDEs的色谱保留时间（RRT）、正辛醇/空气分配系数（lgK_OA）和298 K超冷流体蒸气压（lgP_L）的3个定量构效关系模型。模型复相关系数（R）分别为0.9953、0.9983和0.9982,逐一剔除法交叉验证相关系数（Q）分别为0.9948、0.9975和0.9975,标准偏差（SD）分别为0.0222、0.0754和0.0868,均优于前人的工作。研究结果表明,所建模型具有良好的稳健性和预测能力,拓扑距离特征定位指数对PBDEs性质的表征是有效的。     

氯化1-{2-[双(2-氨基乙基)氨基]乙基}吡啶离子液体的合成及在ATRP反应中的应用

采用N-烷基化方法将二乙烯三胺（DETA）接枝到氯化1-氯乙基吡啶离子液体[CePy]Cl上,合成了离子液体氯化1-{2-[双（2-氨基乙基）氨基]乙基}吡啶（[N₃Py]Cl）,通过FTIR、¹H NMR和MS等测试手段对合成离子液体的结构进行了表征。采用循环伏安法对离子液体配合物[N₃Py]Cl/CuBr和有机配合物PMDETA/CuBr的氧化还原电位（E_1/2）进行测试,结果表明：合成的离子液体[N₃Py]Cl和CuBr形成配合物的氧化还原电势为E_1/2=-0.541V,比常用的有机配合物PMDETA/CuBr（E_1/2=-0.142V）具有更低的氧化还原电势。将离子液体[N₃Py]Cl与CuBr配位形成催化体系,在离子液体[AMIM]Cl中催化甲基丙烯酸甲酯（MMA）的原子转移自由基聚合（ATRP）反应。结果表明,当配体、催化剂和溶剂的用量分别为n（CuBr）=0.19mmol、n（[N₃Py]Cl）=1.13mmol、n（[AMIM]Cl）=0.02mol,反应温度60℃,反应时间4h时,单体转化率高达75%,分子量分布较窄（M_w/M_n=1.24）,ATRP反应具有明显的可控性能。     

量子拓扑指数法预测多氯联苯醚的热力学性质

应用密度泛函理论(DFT),在B3LYP/6-31+G(d)基组上优化和振动分析计算了多氯联苯醚（PCDEs）所有209种可能的分子空间几何结构,得到其各原子之间空间拓扑距离,并建立拓扑空间距离矩阵。结合分子中各原子的支化度,应用原子的平衡电负性对分子图进行着色,得到量子拓扑指数PX₁、PX₂。采用多元线性回归技术建立联苯醚和209种可能结构的多氯联苯醚PCDEs 3种少见报道的热力学性质--标准生成热、标准生成自由能和相对自由能与PX₁、PX₂的定量关系拓扑模型,并用该模型分别对不同热力学性质进行预测与估算。结果表     

四元体系NaCl+NaBO2+Na2CO3+H2O 298.15 K 相平衡研究

柴达木盐湖中具有丰富的盐湖离子,对其中的一个四元体系水盐相图开展研究,采用等温溶解平衡法开展了298.15 K时四元体系NaCl+NaBO₂+Na₂CO₃+H₂O相平衡研究,测定了体系平衡液相组成及密度和折光率,绘制了四元体系NaCl+NaBO₂+Na₂CO₃+H₂O 298.15 K的相图及相应的物化性质图。研究发现NaCl+NaBO₂+Na₂CO₃+H₂O四元体系298.15 K 时包含2个共饱点（E₁、E₂）、5条溶解度曲线（AE₁、BE₁、CE₂、DE₂、E₁E₂）、4个结晶区（NaCl、NaBO₂·4H₂O、Na₂CO₃·7H₂O、NaCl·NaBO₂·2H₂O）。其中三元体系NaCl+NaBO₂+H₂O在298.15 K下产生了复盐NaCl·NaBO₂·2H₂O,通过研究发现该四元体系NaCl+NaBO₂+Na₂CO₃+H₂O在298.15 K下也具有NaCl·NaBO₂·2H₂O复盐区。     

优筋布置矩形箱体应力及变形分析

针对工业生产中矩形箱体笨重、加筋结构布置设计欠佳的问题,采用ANSYS APDL语言对矩形箱体进行静压工况下应力及变形分析。选取6因素5水平正交试验方案,以矩形箱体最大一次应力S_1max、最大等效应力S_2max以及最大变形量Δ_max作为试验指标,侧壁加强铁间距A、宽度B及厚度C,端壁加强铁间距D、宽度E及厚度F作为试验因素,结合矩阵分析法获得加强筋的优筋布置方案A₄B₅C₅D₂E₅F₂,并用ANSYS一阶优化算法对箱壁以及箱壁加强铁壁厚进行优化。结果表明:矩形箱体采用优筋布置后,箱体质量减少了27%。最后采用极限载荷分析法通过P_T=0.1 MPa试验工况验证。     

环境中新型污染物多溴联苯醚的预处理技术及分析方法研究进展

多溴联苯醚是一种新型的持久性有机污染物。本文对其理化性质、污染来源、预处理技术及分析方法等进行了综述,并提出了今后多溴联苯醚的研究方向。     

新能源汽车电池用无镁储氢合金的制备与性能研究

采用真空电弧熔炼和925 ℃/12 h退火的方法制备了Y_1-xLa_xNi_3.25Al_0.15Mn_0.15储氢合金（x=0~1）,研究了x值对储氢合金物相组成和电化学性能的影响。结果表明,x=0和0.15的储氢合金主要由LaNi₅和Ce₂Ni₇相组成,x=0.25、0.33和0.5储氢合金主要由Ce₅Co₁₉和Ce₂Ni₇相组成,x=0.75和1储氢合金主要由PuNi₃、LaNi₅和Ce₂Ni₇相组成;相同充放电循环周次下,x=0.15~1储氢合金的放电容量和抗氢致非晶化能力都高于x=0储氢合金,且随着x从0增加至1,储氢合金的最大放电容量（C_max）、容量保持率（S₁₀₀）、氢扩散系数（D₀）和高倍率放电性（HRD₉₀₀）都呈现先增加后减小趋势,在x=0.33时取得C_max、S₁₀₀、D₀和HRD₉₀₀最大值。Y_1-xLa_xNi_3.25Al_0.15Mn_0.15储氢合金的循环稳定性与合金电极的耐腐蚀性密切相关,高倍率放电性能取决于储氢合金的氢扩散速率。     

Cu-3-trz-PMo12的合成、结构及催化氧化碘离子性能

采用水热法合成了一例新的多酸基有机-无机杂化物,通过X射线单晶衍射、傅里叶变换红外光谱（IR）、热分析测试（TG）、X射线衍射分析（XRD）、扫描电子显微镜（SEM）、元素分析对化合物进行了表征。X射线单晶衍射分析结果表明,化合物的结构式为（PMo₁₂O₄₀） ［Cu₆（C₂H₄N₄）₆］（PMo₁₂O₄₀）?H₂O（简称为Cu-3-trz-PMo₁₂）,属于三方晶系,R-3空间群,晶胞参数a=1.756 66（3） nm、b=1.756 66（3） nm、c=2.303 24（6） nm、α=β=90°、γ=120°、V=6.155 2（3） nm³、Z=3、R₁=0.023 8、wR₂=0.059 2。化合物是由6个3-氨基-1,2,4-三氮唑、6个Cu⁺、两个经典的Keggin型［PMo₁₂O₄₀］^3-及一个间隙水分子组成的二聚体,两个这样的二聚体通过氢键交替相连形成次级单元,每个次级单元之间又通过氢键作用进而形成一个三维超分子结构。催化研究表明,该非均相催化剂在催化过氧化氢氧化碘离子中表现出较为优异的催化活性且具有较稳定的可重复性。     

超薄钯铜纳米片组装纳米花的构建及其氧还原性能

在原子水平上精确调控电催化剂的组成是增强其氧还原（ORR）性能的有效途径。本文采用简单的一步溶剂热还原法制备了由不同PdCu组成的超薄双金属纳米片自组装而成的三维（3D）合金纳米花（Pd₁Cu_x NCFs）。利用透射电子显微镜（TEM）、扫描透射电子显微镜-能谱仪（STEM-EDS）、X射线粉末衍射（XRD）和X射线光电子能谱（XPS）等手段系统表征了Pd₁Cu_x NCFs的形貌、晶体结构及成分。相比于传统二维（2D）纳米材料,Pd₁Cu_x NCFs丰富的快速传质路径、较高的Pd原子利用效率和更强的PdCu双金属间协同作用使得其在碱性介质中表现出增强的ORR性能。另外,本文还研究了Pd、Cu前体用量对ORR性能的影响。结果显示,Pd、Cu前体摩尔比为1∶0.5时,催化剂（Pd₁Cu_0.5NCFs）在碱性介质中ORR活性和电化学稳定性最佳。其半波电位E_1/2（0.937V）远高于商业Pt/C（0.851V）;在加速循环1000次扫描后,E_1/2几乎没有变化,说明其稳定性优异;0.90V电势下,Pd₁Cu_0.5 NCFs的质量比活性为1.09A/mg,是商业Pt/C的14.5倍。     

Theoretical investigation on cyclic reciprocal derivative chronopotentiometry: Kinetic study of totally irreversible electrode processes

Theoretical expressions and mathematical analysis in cyclic reciprocal derivative chronopotentiometry (CRDCP) are presented for totally irreversible electrode processes corresponding to the application of symmetrical and unsymmetrical programmed currents. For two successive unsymmetrical programmed currents, the effect of the currents ratio b (b = |I₂(t)/I₁(t)|) on the (dt/dE)–E curves is discussed. The electrochemical behavior of totally irreversible electrode processes has been studied corresponding to the application of the unique unsymmetrical programmed Φ^m(I₀) proposed recently. CRDCP characteristic parameters obtained for totally irreversible electrode processes are different from those of reversible electrode processes. Therefore, a comparison of CRDCP between both mechanisms is presented. Based on the mathematical derivation, alternative methods for kinetic measuring are described. It is prospected that CRDCP is convenient and applicable for studying the reversibility of the electrode processes in form of CRDCP characteristic parameters.     

The problem of correction for ohmic potential drop in linear potential sweep experiments and the derivation of s0 values for electrode surface processes

Rate constants or exchange current densities of electrode surface processes involving adatom arrays are conveniently evaluated by determining that sweep rate, s₀ (the reversibility parameter), in a linear potential sweep (LPS) experiment, below which the process just remains kinetically reversible, ie its overpotential is sensibly zero. Transition to irreversibility is characterized by peak potentials, E_p, becoming linear in the log of the sweep rate, s, following a region of independence of s for < s₀. A suitable extrapolation procedure enables s₀ to be evaluated. However, if s₀ is large and/or the resistivity of the solution is appreciable, the IR_u drop associated with uncompensated resistance in the measurement system can be comparable with the increase of E_p with log s, when s > s₀, rendering evaluation of s₀ inaccurate. While compensation or empirical correction for this may be made, it is desirable that the nature of the IR_u effect of the LPS I vs E profiles be understood in a more fundamental way. It is the purpose of this communication to provide such a treatment of this effect through evaluation of the actual time-dependent potential that becomes applied to the electrode, and to propose criteria based on the product of s₀, R_u and the reaction pseudocapacitance, C_φ for indicating the anticipated extent of the IR_u effect in the evaluation of s₀. While the transition in the E_p vs log s plot may be due to IR_u effects as well as to kinetic irreversibility, when the former are appreciable, it is shown that the corresponding transition in the value of C_φ with increasing log s can usually allow spurious IR_u and significant irreversibility effects to be distinguished.     

Kinetics of Fischer–Tropsch synthesis on titania-supported cobalt

Rate data have been obtained for CO hydrogenation on a well-characterized 11.7% Co/TiO₂ catalyst in a differential fixed bed reactor at 20 atm, 180–240°C, and 5% conversion over a range of reactant partial pressures. The resulting kinetic parameters can be used to model precisely and accurately the kinetics of this reaction within this range of conditions. Turnover frequencies and rate constants determined from this study are in very good to excellent agreement with those obtained in previous studies of other cobalt catalysts, when the data are normalized to the same conditions of temperature and partial pressures of the reactants. Based on this comparison CO conversion and the partial pressure of product water apparently have little effect on specific rate per catalytic site. The data of this study are fitted fairly well by a simple power law expression of the form −r_CO=kP_H2^0.74P_CO^−0.24, where k=5.1×10⁻³ s⁻¹ at 200°C, P=10 atm, and H₂/CO=2/1; however, they are best fitted by a simple Langmuir–Hinshelwood (LH) rate form −r_CO=aP_H2^0.74P_CO/(1+bP_CO)² similar to that proposed by Yates and Satterfield.     

Simultaneous desulfurization and denitrification of sintering flue gas via composite absorbent

Experiments on simultaneous absorption of SO_2 and NO_X from sintering flue gas via a composite absorbent NaClO_2/NaClO were carried out. The effects of various operating parameters such as NaClO_2 concentration(ms), NaClO concentration(mp), molar ratio of NaClO_2/NaClO(M), solution temperature(TR), initial solution pH, gas flow(Vg) and inlet concentration of SO_2(CS) and NO(CN) on the removal efficiencies of SO_2 and NO were discussed. The optimal experimental conditions were determined to be initial solution pH = 6, TR=55 °C and M = 1.3 under which the average efficiencies of desulfurization and denitrification could reach99.7% and 90.8%, respectively. Moreover, according to the analysis of reaction products, it was found that adding NaClO to NaClO_2 aqueous solution is favorable for the generation of ClO_2 and Cl_2 which have significant effect on desulfurization and denitrification. Finally, engineering experiments were performed and obtained good results demonstrating that this method is practicable and promising.     

Small-angle neutron scattering from branched epoxide resins

Small-angle neutron scattering experiments in the range of q² from 0.01 to 25 nm⁻² have been carried out on branched epoxide resins based on bisphenol-A at the Institute Laue—Langevin (I.L.L) in Grenoble (q=(4π/λ) sin(θ/2)). Measurements were made with six samples in the range of M_W from 1500 to 19 000 and four concentrations between 1.3 and 10% (w/w) in deuterated diglyme. The results are as follows: (i) The mean square radius of gyration follows a relationship S²_z=4.69×10⁻⁴M^1.20_W (nm²). (ii) In all cases fairly large second virial coefficients A₂ are obtained which, however, decrease strongly with molecular weight. Above M_W=2500, the virial coefficient follows the relationship A₂=1.6M^−0.85_W (mol cm³g⁻²). (ii) The reciprocal particle scattering factor as a function of q² exhibits only a slight upturn and otherwise shows the behaviour of a randomly branched polycondensate. The slight upturn is discussed as being caused by the finite volume of the monomeric unit. Possible reasons for the high exponent in the S²_z versus M_W dependence are briefly discussed.     

Electrosorption and inhibition properties of p-norborn2-yl phenolate ions at the mercury/solution interface

The electrosorption properties of p-norborn-2-yl phenolate ions in alkaline solutions were investigated by ac polarographic and electrocapillary measurements.

Two adsorption regions were found. At low bulk surfactant concentrations the adsorption at the positively charged electrode (−0.2 E −0.6 V) is predominant while at higher surfactant concentrations the adsorption at the negatively charged electrode (−0.6 E −1.0 V) is more pronounced. At E = −0.40 V the adsorption parameters were determined (a ≈ 2; ΔG°_A = −32.5 ± 1 kJ mol⁻¹. Between −0.6 E −1.0 V one potential of maximum adsorption for all concentrations does not exist and therefore the adsorption parameters could not be calculated.

At E = −0.40 V progressive two-dimensional nucleation with a nucleation order of 3 was observed which corresponds well with the high attraction constant.

The electrode reaction S₂O²⁻₈ + 2e⁻ → 2 SO²⁻₄ is inhibited by norborn-2-yl phenolate ions in the potential range −0.2 E −0.6 V. In the second potential range of capacity decrease the electrode process is much less retarded. At E = −0.40 V, in a similar manner as described for neutral molecules, a linear dependence of the log k_s (k_s apparent rate constant) on ln c_A and π (π = surface film pressure), respectively, has been found.     

Radiation graft-copolymerization kinetics of poly(ethylene terephthalate) fibres

A theoretical analysis of radiation grafting kinetics has been made in terms of the quantitative interrelationship between the degree of grafting (G_f), the grafting periods (t) grafting temperature (T) and the monomer content in the polymeric system (M). Poly(ethylene terephthalate) fibres and a number of hydrophilic monomers have been employed for these experiments. The grafting reactions were initiated by trapped radicals produced by irradiation of the polymeric system under vacuum at room temperature. Experimental results showed that the monomer content in the fibres obeyed the Arrhenius relationship. The overall activation energy of the grafting reaction has been calculated. Grafting reactions can proceed only if ΔE_t > ΔE_p + ΔE_M. This termination activation energy ΔE_t is a function of the state of polymeric system.     

Effect of macromolecular length on anisotropic scattering of light in an electric field

Light scattering by monodisperse solutions of rigid rod-like anisotropic macromolecules, with linear dimensions l of the order of incident wavelength λ, oriented in an external d.c. electric field, →E has been analysed. The relative variations δV^E_v, δH^E_v, δV^E_h, δH^E_h of the scattered light components are discussed for the three values [l/λ] = 1, 0·5, 2, and various reorientation parameters, p = [μE/kT] of the permanent dipole moment μ and q = [(₃ − ₁)E²/2kT] of the moment induced by the principal polarizabilities ₁ = ₂ ≠ ₃. The saturation orientation field strength has been calculated for certain macromolecules with the aim of determining their optical anisotropy numerically.     

Determination of the optimum conditions for the cementation of cadmium with zinc powder in sulfate medium

The orthogonal array design has been used to determine the optimum conditions for the cementation of cadmium from a synthetic zinc sulfate solution and hence to achieve the highest cementation efficiency and the best robustness of the quantitation from the least number of trials in a laboratory scale. Cementation was performed using zinc powder. The orthogonal array L₉ (3⁴) that comprises four parameters at three levels was chosen. The parameters and their levels were as: zinc powder quantity (Z): 1, 1.2 and 1.5 times of stoichiometric quantity of cadmium; time (t): 4, 8 and 12 min; temperature (T): 25, 35 and 45 °C and zinc powder particle size distribution (R): nos. 1–3. The ultimate optimum cementation conditions were found to be Z₁ (equal to stoichiometric quantity of cadmium), T₁ (25 °C), R₃ (no. 3) and t₁ (4 min). Under these conditions, cementation percentages for cadmium and nickel were 95.83% and 6.63%, respectively.