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901.
BaCe1—xRExO3—0.5x的溶胶—凝胶法合成及离子导电性   总被引:3,自引:0,他引:3  
何志奇  蒋凯 《应用化学》1998,15(3):22-25
用溶胶-凝胶法合成了系列钙钛矿结构的BaCe1-xRExO3-0.5x(RE=La,Nd,Sm,Eu,Gd,Dy,Ho,Er和Y)复合氧化物,通过XRD和热分析对样品结构及生成过程进行了研究.测定了不同温度下样品的交流阻抗谱,讨论了稀土离子掺杂对BaCeO3电性质的影响.溶胶-凝胶法比固相反应法合成温度降低了600~800℃,稀土掺杂使BaCeO3离子导电率提高了10~40倍.  相似文献   
902.
非均相羰基氧化合成碳酸二苯酯反应液组分的分析   总被引:6,自引:0,他引:6  
通过色质联用仪对非均相催化一步合成碳酸二苯酯(DPC)过程中的反应液的主要产物及副产物进行了定性分析,其结果发现该反应的主要副产物为苯氧基丙酸和4-苯氧基苯酚以及四丁基铵盐;用气相色谱外标法对反应液中的DPC进行了定量分析,并通过回归法得到了定量分析:DPC的计算方程式,实验证明该方程在DPC的浓度小于10%范围内比较可靠。  相似文献   
903.
SnO2/Al2O3 catalyst prepared by sol-gel method showed higher activity than those prepared by impregnation method, and their activity was significantly improved by pre-treatment in the reaction gas. The increased activity is closely related to the agglomeration of SnO2 species and the re-exposure of Al2O3, which was previously covered by dispersed SnO2 species. This revised version was published online in June 2006 with corrections to the Cover Date.  相似文献   
904.
We demonstrate, both theoretically and experimentally, that it is possible to use an electric field to drive the formation of macroscopic chiral (conglomerate) domains from an initially homogeneous fluid racemate. Field-induced segregation is exhibited in a fluid smectic liquid-crystal phase of a racemic mesogen, wherein enantiomerically-enriched domains are readily identifiable by their chiral electro-optical response. The sharp field-generated boundaries that form between opposite-handed domains broaden by diffusion in the absence of field, but reform rapidly if the field is switched on again, providing unambiguous evidence for the field-driven physical separation of enantiomers. A mean-field model successfully describes the steady-state and the dynamic evolution of conglomerate formation.  相似文献   
905.
郭丽  虞忠衡  朱士正  陈庆云 《化学学报》2005,63(10):897-902,i002
用密度泛函理论研究了CF3SO3CF2CF3 F^-的碳氧键断裂反应的机理。首先,用DFT方法优化了反应物、中间体、过渡态、产物的平衡构型,分析了碳氧键断裂反应的势能面变化,发现在SN2反应机理中,除了S-O断裂SN2反应外,引起C-O键断裂的同面进攻也是一个可能的反应途径。理论计算表明,最终反应的产物是受热力学控制的,S-O键的断裂绝对地优于C-O的断裂。因此,C-O断裂的同面机理虽然是可能的,但却难以被实验观察到,本文还讨论了端基-CF3在同面SN2反应中的邻位效应,以及基组对这个效应的影响。  相似文献   
906.
溶胶凝胶法制氧化铝负载铜基超细粒子催化剂的研究   总被引:9,自引:1,他引:9  
雷翠月  陈霄榕 《分子催化》1998,12(5):375-380
采用溶胶凝胶法制氧化铝负载铜基超细粒子催化剂的制备了氧化铝负载的铜基超细粒子催化剂,用TG-DTA,XRD,BET以及TEM等技术手段,对催化剂的物相结构,表面孔结构,粒子形貌以及催化性能等进行了研究。结果表明,利用溶胶凝胶法,可以直接帛备出高比表面积,低堆积密度的纤维状纳米级负载型Cu/Al2O3超细粒子;活性组分以远低于纳米级的微晶粒子簇状态,均匀地分散在纳米级氧化铝载体表面上,而且在低于50  相似文献   
907.
任意多阶梯度场强毛细管凝胶电泳中谱带的迁移和展宽   总被引:2,自引:0,他引:2  
在自行制备的毛细管凝胶电泳柱上,通过实验考察毛细管凝胶电泳(CGE)中场强(E)和组分迁移率(μ)的关系,发现在一般CGE使用的场强范围内,μ随E增大而成近似线性的增加。并讨论了产生这种现象的原因。以此为基础提供了任意多阶梯度场强毛细管凝胶电泳中组分的迁移时间和距离的计算公式,用于编制计算机程序。  相似文献   
908.
The molecular improved generator coordinate Hartree–Fock (MIGCHF) method is used to generate accurate basis sets of primitive Gaussian-type functions for the H2O molecule. Sequences of increasing size atom centered basis sets are employed to explore the accuracy that can be achieved with this method. Using the O(24s14p8d5f2g1h);H(22s9p5d2f1g) basis set, the HF and second-order electron correlation energies of the H2O ground state at the experimental geometry are computed as −76.0674680 and −0.3491935 hartree, respectively. The HF energy is in error by 20 μhartree and the second-order correlation energy corresponds to 96.5% of an estimate of the limiting value. The relevance of the present calculations is to show the accuracy that can be achieved in studies of small polyatomic molecules with the MIGCHF method.  相似文献   
909.
Summary The results of a wide-ranging investigation into some of the different methods available for performing the joining of templates to build molecular models show that the choice of algorithm can significantly affect the quality of the results obtained, and different algorithms are most suited to particular categories of join.  相似文献   
910.
A study has been undertaken of stress relaxation in ovalbumin thermotropic gels with a concentration of 8–20%, depending on time and temperature of heating (respectively, 20–60 min, 70°–110°C), at pH 2.5–10.0. In all instances, the dependence of the initial gel elasticity modulus on heating has a single maximum. Gelation conditions corresponding to this maximum are considered optimal. Optimal gelation time is 30 min, regardless of pH. On the other hand, the optimal heating temperature depends on pH. To the right and left of the isoelectric point of protein (2.5pH<4.0 and 5.5G) of gels on heating conditions, pH and protein concentration (X 1,X 2,X 3,X 4), as well as on time of relaxation (t) may be generally described asG(X 1,X 1,X 1,X 1,t)=G e(X 1,X 2,X 3,X 4)f(t), whereG e is the equilibrium value of the elasticity modulus, and f(t) the relaxation function. Thus, a change in the parameters only affects the value of the equilibrium elasticity modulus, and exerts no effect on the relaxation time spectrum. For this reason, all the relaxation curves obtained may be transformed into two normalized relaxation functions:f(t)=f(t)/f(1)=G(X 1,X 2,X 3,X 4,t)/G(X 1,X 2,X 3,X 4, 1)Each of these normalized functions corresponds to one of the homologous groups. Rheological similarity of gels in each homologous group evidently points to their structural similarity. Invariance of the gel relaxationproperties with regard to protein concentration, leads to a concentration dependence of the equilibrium modulus at various pH values. These dependences are curvilinear on a double logarithmic scale. The slope of the curve exceeds 2 in the entire concentration interval studied. In other words, the dependences obtained cannot be described by the usual law of squares. On the other hand, they adequately match Hermans theoretical relation for a network formed by random association of identical polyfunctional particles without cyclization. This simple model evidently gives a true picture of the major regularities of thermotropic gelation for ovalbumin. An agreement between this theory and experiment was achieved for a protein concentration ofC *=6.0±1.0% at the gel point regardless of pH. Invariance of gelpoint position with regards to pH demands further confirmation.List of symbols T h,t h heating temperature and time - T h * ,t h * optimal heating temperature and time - C protein concentration - C * protein concentration in gel-point - G relaxation modulus - G e equilibrium modulus - f(t) relaxation function - t time of relaxation - f(t) normalized relaxation function - fT A (t), f B (t) normalized relaxation functions of groups A and B - G 1 T h,t h-reduced modulus - G 2 T h,t h, pH-reduced modulus - G 3 C-reduced modulus - b 1 T h, th reduction parameter of modulus - b 2 pH reduction parameter of modulus - b 3 C reduction parameter of modulus - Wg gel-fraction  相似文献   
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