有规立构聚苯乙烯的稀溶液性质

本文报导了有规立构聚苯乙烯,无规立构聚苯乙烯和1∶1混合有规和无规立构聚苯乙烯的分级、粘度和光散射测试结果。发现上述三种聚苯乙烯试样的[η]-M的依赖关系、第二维利系数和均方末端距(当分子量相同时)是有差别的。这种差别超出实验误差范围,而作者们认为是合理的。从而讨论了前人在类似的工作中所得到的结果。     

共混高聚物的混溶性研究(摘要)

在此介绍马萨诸塞州立大学在共混高聚物方面的研究工作。这些共混高聚物可分为三类:(1)非晶—非晶,如PCL(聚己内酯)(<50％)/PVC(聚氯乙烯);(2)结晶—非晶,如PCL(>50％)/PVC、i-PS(全同立构聚苯乙烯)/PPO(聚苯醚)、i-PS/α-PS(无规聚苯乙烯)、PVF_2(聚偏氟乙烯)/PMMA(聚甲基丙烯酸甲酯);(3)结晶—结晶,如PBT(聚对苯二甲酸丁二酯)/PET(聚对苯二甲酸乙二酯)。为研究第一类非晶共混物的混溶性,以 PCL/PVC     

聚苯乙烯序列分布链长依赖性的13C NMR研究

高分子序列分布对于研究聚合机理以及聚合物结构与性能的关系有重要意义．１３ＣＮＭＲ谱是研究聚合物序列分布的常用方法．无规立构聚苯乙烯（ａＰＳ）各谱峰的归属及其序列分布已有许多报道［１３］．然而对于分子量低于１０４的ａＰＳ齐聚物和低聚物的序列分布研究却少...     

无规聚苯乙烯在稀溶液中的急冷结晶

通常认为聚苯乙烯具有立体规整度的构型才能结晶,无规聚苯乙烯一般不能结晶。我们用液氮急冷浓度低于体积收缩浓度的无规聚苯乙烯溶液,再将溶剂在真空中升华,得到的粉末状样品含有六角晶系的多晶及单晶。这一发现对研究高分子聚集态结构有重要意义。     

结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响

本文通过核磁氢谱、DSC和分子量测定,研究了结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响.分子量测定的结果表明,等规立构聚甲基丙烯酸甲酯结晶后,其辐射裂解反应减弱,裂解G值减小将近一半.核磁氢谱测定辐照试样的空间立构变化结果为:随着辐照剂量的增加,等规立构逐渐变为无规立构和间规立构,其变化规律相似于非晶试样.结果还表明,晶区的消旋反应比裂解反应更为显著.DSC测得的试样熔点,随着辐照剂量的增加而急剧下降,由Flory结晶熔化理论计算得晶区的辐射破坏G值为8.8.该值远大于聚乙烯晶区的破坏G值.     

结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响

 本文通过核磁氢谱、DSC和分子量测定,研究了结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响.分子量测定的结果表明,等规立构聚甲基丙烯酸甲酯结晶后,其辐射裂解反应减弱,裂解G值减小将近一半.核磁氢谱测定辐照试样的空间立构变化结果为:随着辐照剂量的增加,等规立构逐渐变为无规立构和间规立构,其变化规律相似于非晶试样.结果还表明,晶区的消旋反应比裂解反应更为显著.DSC测得的试样熔点,随着辐照剂量的增加而急剧下降,由Flory结晶熔化理论计算得晶区的辐射破坏G值为8.8.该值远大于聚乙烯晶区的破坏G值.     

聚甲基丙烯酸甲酯辐射裂解和消旋的空间立构效应

本文研究了三种不同空间立构聚甲基丙烯酸甲酯的辐射效应,提出裂解过程是一种裂解与重合的动态平衡过程。分子量降低和消旋作用对温度的依赖性,是由于分子运动和笼罩效应以及重合的空间位阻效应所致。辐照温度愈高,裂解产额愈大。相同条件下辐照,全同立构比无规立构试样的裂解产额更大。 全同立构聚甲基丙烯酸甲酯辐照后,不仅分子链断裂,而且空间立构也发生很大变化。随着辐照剂量的增加,全同立构含量逐渐减少,而无规立构含量和间同立构含量却逐渐增加。     

基底表面无规聚甲基丙烯酸甲酯立构复合结构的研究

采用原子力显微镜和反射吸收红外光谱研究了在基底上无规聚甲基丙烯酸甲酯立构复合结构的形成和结构特征,纯等规和间规聚甲基丙烯酸甲酯与等规/间规混合物(有立构复合结构生成)表面聚集形貌比较的结果表明,立构复合结构的生成使聚甲基丙烯酸甲酯在基底上形成树枝状的聚集形貌,因此无规聚甲基丙烯酸甲酯在基底上的树枝状聚集形貌表明了其内部生成了立构复合结构,而且这种结构对聚集形貌产生了重大影响,反射吸收红外光谱的研究表明,在基底表面薄膜中无规聚甲基丙烯酸甲酯主链结构比在本体厚膜中的更加伸展,更有利于立构复合结构的生成.     

iPP／aPP共混物溶液浇铸薄膜的形态结构研究

用透射电子显微镜和Ｘ射线衍射等方法研究了等规立构聚丙烯和无规立构聚丙烯共混物溶液浇铸膜的形态结构，结果表明，ａＰＰ的加入对ｉＰＰ的形态结构有很大的影响。     

T_g以下温度退火对无规聚苯乙烯性能的影响

用调幅式ＤＳＣ等新技术研究了物理老化对无规聚苯乙烯多种性能的影响．随着老化时间的延长，试样的玻璃化转变温度、热焓松弛、峰温、峰高和热焓提高；老化使材料的初始模量，屈服应力和断裂强度都有不同程度的提高；使样品的溶剂扩散速率降低，但对样品的密度和声传播速度几乎没有影响．以上这些结果可从物理老化引起试样中凝聚缠结增加的观点来进行解释．     

膜渗透计测定低分子量聚合物

本文用小体积膜渗透计及动态渗透压法测定了聚苯乙烯标准样品(分子量1000—17000)和一系列主链含-5氟尿嘧啶聚酯的分子量(低于9000)。同时研究了再生纤维素玻璃纸制备的半透膜的渗透性和选择性。该膜在丙酮中具有较高的选择性,可测定1000分子量。 低分子量聚苯乙烯的第二维利系数A_2依从A_2=常数·(?)关系。     

IR STUDY ON MONOMOLECULAR PARTICLE AGGLOMERATES OF POLYSTYRENE OBTAINED BY FREEZE-DRYING OF ITS DILUTE SOLUTION

The monomolecular particle agglomerates of polystyrenes were obtained by freeze-drying of its very dilutesolutions of 1.3×10~(-5)-2.0×10~(-5) g/mL in benzene: cylcohexane (100:1) solvents, and they were annealed at roomtemperature for hundred days before use. According to ~(13)C-NMR measurement the polystyrenes should be practically atactic.The number average molecular weights of the samples are 2.80×10~3, 2.00×10~4, and 1.55×10~6, respectively. The freeze-dried aPS with a molecular weight higher than 10~4 show two new IR absorption bands at 1098 and 1261 cm~(-1), which areabsent in the normal aPS and freeze-dried styrene oligomer. It was also found that the low molecular weight samples canonly form powders, whereas the freeze-dried aPS with higher molecular weight form a mixture of powders and fibrils, ofwhich the longer fibrils show a much stronger 1261 cm~(-1) band than the shorter fibrils and the powder. It seems that the1261 cm~(-1) band corresponds to the stacking behavior of monomolecular particles.     

Molecular-weight fractionation of polystyrene by zone-melting chromatography

Polystyrene can be fractionated by zone-melting chromatography on a solid column of durene. The polymer solute moves in the same direction as the heated zone. The higher the molecular weight of the polymer the slower it moves. Experiments with model mixtures of monodisperse polystyrenes of average molecular weight 6 x 10(2)-2 x 10(5) indicate that a polymer fraction can be separated in 90% purity from fractions with molecular weights higher or lower by one order of magnitude. Polystyrene samples of various molecular weight distributions, after processing on durene columns, gave several fractions having significantly narrower dispersions than that of the starting polymer, in terms of gel-permeation chromatography.     

邻-酚羟基取代N-杂环卡宾[C,O]螯合双配体镍/MAO催化降冰片烯加成聚合的研究

3种邻-酚羟基取代的N-杂环卡宾[C,O]螯合双配体镍配合物在甲苯中以甲基铝氧烷(MAO)为助催化剂,催化降冰片烯(NBE)聚合.考察了反应温度、时间、n(Al)/n(Ni)以及n(NBE)/n(Ni)等因素对催化活性和所得聚降冰片烯相对分子质量及其分布的影响.结果表明,0℃时催化体系的聚合活性可达,1.34×107gPNBE/(molNi.h);所得聚降冰片烯(PNBE)重均相对分子质量(Mw)可达2.0×106,相对分子质量分布(Mw/Mn)为3.3~1.5,热分解温度在440℃附近,且在室温下可溶于环己烷和三氯苯.通过对聚合产物FTIR,13C-NMR和WAXD分析表明,该聚合反应以烯烃加成聚合方式进行,且聚合物是非晶态结构.     

Method of determination of dielectric relaxation characteristics of plasticized polystyrenes on the basis of calorimetric glass temperature

The dielectric loss measurements of different polystyrenes (fractions and blends) with different molecular weights (M _n 2000–125000 g/mol) were carried out in the frequency range 10^–2–10⁶ Hz and the temperature range of the glass process (60°–135°C, depending on the molecular weight). The measurements of the pure fractions showed that the half-width of the glass relaxation process of the different polystyrenes can be correlated by a straight line, if they are plotted versus the relaxation frequency maxima of the glass process, regardless of the difference in both their molecular weight and glass transition temperature. Moreover, the fine structure of the shape of the glass process of polystyrenes with different molecular weights was found to be the same when the glass process appears at the same relaxation frequency range. The addition of oligostyrenes or low molecular <10% wt additives to the high molecular weight polystyrene did not influence the shape of the glass process. The calorimetric glass transition temperature of polystyrene was found to be only dependent on the number average molecular weight as well as on the number of end groups, but not on the molecular weight distribution. The obtained experimental results were correlated to develop a method for the estimation of the dielectric relaxation characteristics (relaxation frequency as well as the shape parameters) of the glass process of plasticized polystyrenes based on the calorimetric glass transition temperature. A method for the analysis of the dielectric relaxation curves of mixtures of label and polymer is suggested.     

不同分子量尼龙1010的结晶与熔融

不同分子量尼龙１０１０的结晶与熔融＊朱诚身王经武王友文杨桂萍（郑州大学材料工程系郑州４５００５２）陈玉莫志深（东北师范大学分析测试中心长春１３００２４）（中国科学院长春应用化学研究所长春１３００２２）关键词尼龙１０１０，分子量，结晶，熔融＊１９９４＿...     

灵芝子实体水溶性多糖的分离和分子量测定

用磷酸盐缓冲液、热水、碱和热碱水分别从灵芝子实体分离出五种水溶性杂多糖ＧＬ１、ＧＬ２、ＧＬ３、ＧＬ４和ＧＬ５．紫外光谱、红外光谱、气相色谱及硫酸咔唑分析结果表明，它们主要由葡聚糖、木糖、甘露糖、半乳糖组成，ＧＬ３、ＧＬ４和ＧＬ５含葡萄糖醛酸．由粘度、光散射和膜渗透压法测定了特性粘度［η］、重均分子量Ｍｗ及数均分子量Ｍｎ，ＧＬ２、ＧＬ３和ＧＬ５多糖的Ｍｗ值分别为１２４×１０４、１２８×１０４和５８×１０４．实验结果表明这些杂多糖含水溶性Ｄ 葡聚糖，并且初步推断，用磷酸盐缓冲液提取出的杂多糖ＧＬ２中包含刚性链β Ｄ 葡聚糖     

Three‐Dimensionally Ordered Macroporous Syndiotactic Polystyrene: Preparation and Characterization

Summary: Three‐dimensionally ordered macroporous (3DOM) syndiotactic polystyrenes with pore size in the range of 71–286 nm were fabricated by means of silica templates using (dbm)₂Ti(OPh)₂/MAO catalytic system. The resulting materials were characterized by NMR, SEM, powder X‐ray diffraction, GPC and DSC. The results indicated that the 3DOM syndiotactic polystyrenes were highly syndiotactic, and the pore contraction increased when the average pore diameter decreased. Compared with bulk syndiotactic polystyrenes, 3DOM syndiotactic polystyrene possessed lower molecular weight, narrower molecular weight distribution, and lower crystallinity and melting temperature.

SEM image of 3DOM syndiotactic polystyrene, the inset shows the detail of the cavities.     

星形聚苯乙烯的玻璃化转变温度和液1-液2松弛

用扭辫仪(TBA)和线膨胀仪测定了一组规则的星形聚苯乙烯的玻璃化转变温度T_g和T_ll松弛。两种实验方法的结果表明:支链分子量相同的星形结构聚合物的T_g随着支化度增加而升高,但也发现星形聚苯乙烯的T_g却低于具有相同分子量的线形聚苯乙烯的T_g·液₁-液₂松弛温度T_ll和损耗峰的强度也依赖其支化度。与以二乙烯基苯为凝胶核的星形结构相比较,证实了后者的双T_g转变。     

Multiple melting behavior of poly(butylene succinate). I. Thermal analysis of melt‐crystallized samples

The multiple melting behavior of poly(butylene succinate) (PBSu) was studied with differential scanning calorimetry (DSC). Three different PBSu resins, with molecular weights of 1.1 × 10⁵, 1.8 × 10⁵, and 2.5 × 10⁵, were cooled from the melt (150 °C) at various cooling rates (CRs) ranging from 0.2 to 50 K min^?1. The peak crystallization temperature (T_c) of the DSC curve in the cooling process decreased almost linearly with the logarithm of the CR. DSC melting curves for the melt‐crystallized samples were obtained at 10 K min^?1. Double endothermic peaks, a high‐temperature peak H and a low‐temperature peak L, and an exothermic peak located between them appeared. Peak L decreased with increasing CR, whereas peak H increased. An endothermic shoulder peak appeared at the lower temperature of peak H. The CR dependence of the peak melting temperatures [T_m(L) and T_m(H)], recrystallization temperature (T_re), and heat of fusion (ΔH) was obtained. Their fitting curves were obtained as functions of log(CR). T_m(L), T_re, and ΔH decreased almost linearly with log(CR), whereas T_m(H) was almost constant. Peak H decreased with the molecular weight, whereas peak L increased. It was suggested that the rate of the recrystallization decreased with the molecular weight. T_m(L), T_m(H), T_re, and T_c for the lowest molecular weight sample were lower than those for the others. In contrast, ΔH for the highest molecular weight sample was lower than that for the others. If the molecular weight dependence of the melting temperature for PBSu is similar to that for polyethylene, the results for the molecular weight dependence of PBSu can be explained. © 2002 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 40: 2411–2420, 2002