HIGH PRECISION AUTOMATIC CAPILLARY VISCOMETER

An automatic capillary viscometer with optical fibres as cold light source and a thermostat in which the temperature can be regulated within ±5×10~(-4)℃have been developed for the determination of flow time with an accuracy of ±4×10~(-3) sec. The basic principle, construction, specifications as well as the main features of this instrument are described.     

掺硼多晶金刚石膜的电化学性能研究

采用EACVD(Electron Assisted Chemical Vapor Deposition)方法制备了掺硼金刚石膜, 并用扫描电镜、拉曼光谱及霍尔效应等测试方法对其表面形貌、生长特性、载流子浓度以及导电性能进行了分析. 测试结果表明, 掺硼金刚石膜是由微米级晶粒组成的多晶膜, 其载流子浓度为4.88×1020 cm-3, 电阻率为0.03 Ω·cm, 是高品质金刚石膜. 用该金刚石膜制作电化学电极, 利用循环伏安法分别测量了金刚石膜电极在氯化钾空白底液、亚铁氰化钾溶液和左旋半胱氨酸溶液中的循环伏安曲线, 发现该金刚石膜电极在水溶液中具有宽的电化学窗口(约为3.7 V)和接近零的背景电流, 在生物制剂的检测中具有很高的灵敏度和良好的稳定性, 是一种理想的电化学电极材料.     

苯羧酸气相色谱分析中的鬼峰效应

在气相色谱分析中,直接进样分析苯羧酸有一定困难,通常必须将其制备成衍生物。Kaufman认为,这是由于它们在高温下不能完全挥发,易于脱羧或形成酸酐。Tpycoв研究了o-甲基苯甲酸的直接进样分析,发现汽化室温度超过300℃时有峰的拖尾或消失现象,也怀疑是由于脱羧引起。我们的实验结果表明,苯甲酸、苯乙酸、o-、m-、p-甲基苯甲酸、邻苯二甲酸及水杨酸等苯羧酸,汽化室温度即使超过300℃也     

非晶态Co-B的局域电子结构的X_α原子簇计算

金属玻璃TM-Met(TM为过渡金属原子,Met为类金属原子,如硼、磷等)由于其优异性能已成为非晶态研究的重要课题之一。实验研究表明,类金属原子与过渡金属原子构成非晶态合金(即金属玻璃)后,平均原子磁矩随Met的含量在一定范围内的变化呈线性下降关系.相当多的文献用“电荷转移刚性能带”模型来解释.认为金属玻璃的能带是     

分散介质和表面活性剂对γ-Fe_2O_3/聚丙烯酸锂复合微粒电流变效应的影响

采用反乳液聚合方法制备了γ－Ｆｅ２Ｏ３／聚丙烯酸锂复合微粒，将其悬浮分散于硅油、液体石腊等绝缘介质中形成电流变体。考察了在直流和交变电场作用下分散介质的种类、表面活性剂种类及用量等对复合微粒电流变效应的影响。     

四硫富瓦烯衍生物/硬脂酸LB膜的导电性研究

报导了14种四硫富瓦烯衍生物／硬脂酸LB膜的导电性，并解释了硬脂酸量和碘蒸气掺杂对LB膜导电性的影响．     

六次甲基四碲富瓦烯二碘盐的合成、晶体结构及其某些固态物性

在两相混合溶液中电解合成了HMTTeF·I_2盐的单晶。晶体属P2_1/n空间群,独立区里有一个HMTTeF分子,离子化发生在分子中的一个碲原子孤电子对上。粉末压片常温电导率为4.1×10~(-5)Scm~(-1)。喇曼光谱测定与电导率及X射线分析结果相符。     

CRYSTAL STRUCTURE OF NEODYMIUM（Ⅲ）COMPLEX WITH1，2，4—BENZENETRICARBOXYLIC ACID

<正> [NdC6H3(COO)3(H2O)3]·H2O, Mr=423. 45, orthorhombic,space groupP212121,a=6. 120(3) ,b=9. 719(2) ,c=20. 133(8) A ,V=1197. 5A3.Z = 4,F (000) = 820,DC=2. 35g/cm3,μ(Moka) = 44. 1cm-1.The final R = 0. 0278 and Rw= 0. 0270 for 1760(I>3σ(I)) observed unique reflections. The neodymium ion is nine-coordinated by six oxygen atoms of carboxylato groups from four 1, 2, 4-benzenetricar-boxylates and three aqua molecules,forming a distorted monocapped square antiprism. The Nd -O distances fall in the range of 2. 41 - 2. 70A with an average of 2. 51A     

DETERMINATION OF BRANCHING DISTRIBUTION IN HIGH cis-1,4-POLYBUTADIENE BY GPC AND AUTOMATIC VISCOMETRY

Based on the methods reported by Ambler and Kraus, a method has been developed for the determination of long-chain branching distribution in polymers by the combined use of GPC and intrinsic viscosity data of polymer fractions. In this method, g_i, λ_i, G_i, m_i, the weight percentage of polymer that is branched, etc. can be used simultaneously to characterize the distribution, degree and content of branching in polymers. Some relations between molecular weight polydispersity and branching polydispersity in Nickel-based high cis-1,4-polybutadiene samples are discussed. It was found that the number of long branches λ. per unit molecular weight is a function of molecular weight and all of the samples are highly branched at a molecular weight of about 10~6.