磺酰化修饰聚苯乙烯的合成及芳香烃萃取性能简

利用自由基聚合反应合成了低分子量聚苯乙烯,经过端基氧化和磺酰化反应,制备出一系列极性砜基修饰的低分子量聚苯乙烯. 通过红外光谱(FTIR)、核磁共振谱(NMR)、差示扫描量热分析(DSC)以及热重分析(TGA)等手段对聚合物的结构和性能进行了表征,并通过混合烃萃取分离实验对其芳香烃选择性进行了测试. 结果表明,随着磺化比例的增加,甲苯的选择系数和分布系数均显著提高,表明极性修饰聚苯乙烯对多种芳香烃/链烷烃混合物均具有明显的芳香烃选择性.     

磺酰化修饰聚苯乙烯的合成及芳香烃萃取性能

利用自由基聚合反应合成了低分子量聚苯乙烯, 经过端基氧化和磺酰化反应, 制备出一系列极性砜基修饰的低分子量聚苯乙烯. 通过红外光谱(FTIR)、 核磁共振谱(NMR)、 差示扫描量热分析(DSC)以及热重分析(TGA)等手段对聚合物的结构和性能进行了表征, 并通过混合烃萃取分离实验对其芳香烃选择性进行了测试. 结果表明, 随着磺化比例的增加, 甲苯的选择系数和分布系数均显著提高, 表明极性修饰聚苯乙烯对多种芳香烃/链烷烃混合物均具有明显的芳香烃选择性.     

再生纤维素膜对聚苯乙烯的截留性

本文用铜氨法以及微相分离和后处理技术制备了孔径30A至1000A的一系列再生纤维素膜。采用膜渗透计按流动速率法及静态渗透压法分别测定了它们的平均孔径2rf以及膜在甲苯溶液中对聚苯乙烯标样的截留率Re。得到膜平均孔径和所截留聚苯乙烯分子最Mw及其均方根末端距〈h~2〉~(1/2)之间的关系式分别为: lg2r?=lg0.155 0.59lgM_w lg2rf=lg0.589 0.96lg〈h~2〉~(1/2)     

单茂钪催化合成高顺式异戊二烯/苯乙烯共聚物的研究

合成了5种单茂双烷基稀土配合物Cp'Ln(CH2C6H4NMe2-o)2(1:Cp'=C5Me4Si Me3,Ln=Sc;2:Cp'=C9H7,Ln=Sc;3:Cp'=C5H5,Ln=Sc;4:Cp'=C5H5,Ln=Lu;5:Cp'=C5H5,Ln=Y)在助剂[Ph3C]-[B(C6F5)4]的活化下,考察了稀土金属和配体结构对异戊二烯和苯乙烯的均聚合活性和立体选择性的影响规律.结果表明小空间位阻的单茂钪(C5H5)Sc(CH2C6H4NMe2-o)2(3)催化异戊二烯聚合时,聚合活性和顺式立体选择性较优;催化苯乙烯聚合时获得无规聚苯乙烯.因此选用单茂钪催化剂3/[Ph3C][B(C6F5)4],考察了其催化异戊二烯/苯乙烯共聚合的性能,高活性地获得了组成和分子量可控、分子量窄分布的异戊二烯/苯乙烯多嵌段共聚物.通过1H-NMR,13C-NMR,GPC以及DSC对共聚物进行分析表征,结果表明,通过调控苯乙烯与异戊二烯的加料比例,共聚物中苯乙烯摩尔含量可以在1%~75%间调控,聚苯乙烯嵌段为无规聚苯乙烯;共聚物中聚异戊二烯顺-1,4选择性均大于91%;通过调控单体与催化剂的比例,共聚物分子量(Mn)可以在3.5×104~8.3×104间调控,分子量分布保持窄分布(Mw/Mn=1.71~1.94).     

两亲性嵌段共聚物PS-b-PMAA的合成与胶束化行为研究

利用原子转移自由基聚合法(ATRP)得到了分子量可控、分子量分布接近1.1的聚苯乙烯-b-聚甲基丙烯酸叔丁酯(PS-b-PtBMA)嵌段共聚物, 进而在酸性条件下由水解反应得到了两亲性的聚苯乙烯-b-聚甲基丙烯酸 (PS-b-PMAA)嵌段共聚物．用GPC, FTIR和¹H-NMR等对产物的分子量和组成进行了表征．使PS-b-PMAA在选择性溶剂中进行自组装, 通过激光光散射和透射电子显微镜研究了影响其胶束化行为的因素与胶束形态, 并初步探讨了胶束形成的机理, 发现通过控制嵌段共聚物的链段长度之比可得到空心球形的高分子胶束．     

短链聚苯乙烯稀溶液粘度及渗透压行为

本文用动态膜渗透压及粘度法测定了短链聚苯乙烯的分子量Mn, 第二virial系数A2及特性粘数[η], 得到聚苯乙烯(2.5×10^3, 均方末端距以及扩张因子αs均与报道值一致。本工作表明, 分子量大约在400-1.5×10^4之间, 为聚苯乙烯从小分子到高分子的过渡区, 此时短链聚苯乙烯以蠕虫形链存在于溶液中。     

聚苯乙烯分子链构象与其薄膜的玻璃化转变行为

本文利用椭偏仪研究了成膜方式对不同分子量聚苯乙烯(PS)超薄膜玻璃化转变行为的影响.发现PS超薄膜的玻璃化转变温度(Tg)随着厚度降低的幅度与其成膜方式、分子量有关.当PS膜低于一定厚度时,旋涂法制备的PS膜的Tg比相同厚度浇铸法制备的膜低,且二者Tg差值随着厚度的降低而增大.这二种膜Tg的差值和Tg发生偏离时膜的临界厚度随聚苯乙烯分子量的增加而增加.利用非辐射能量转移荧光光谱证实成膜方式主要是影响PS分子链在膜中的构象.旋涂法制备的PS膜相对于本体在近表面区域分子链的形变更大.分子量愈大,分子运动时内摩擦阻力愈大,近表面区域分子的残余应力愈大.由于强运动能力的活性层(空气/PS界面)对PS薄膜Tg的影响占主导,相同厚度下分子链愈伸展,残余应力越大,PS薄膜的Tg越低,导致成膜方式与分子量的影响也愈大.     

随机支化过程理论与分子量分布函数

本文运用随机支化过程理论于多元反应体系,应用矢量变量、矢量概率再生函数及关于函数Lagrange多元展开的一项定律,简捷地推导了A_(a_1)+A_(a_2)+…+A_(a_i)及A_(a_1)+A_(a_2)+…+A_(a_i)+B_(b_1)+B_(b_2)+…+B_(b_i)两种一般化反应类型的分子量分布函数,结果与Stockmayer用组合理论所得结果相同。本文所用方法较之采用图论的推导方法为简便。     

含无规共聚组分的两嵌段聚合物A-b-(B-r-C)的合成以及自组装

通过原子转移自由基(ATRP)方法合成了其中一个嵌段是由2种单体无规共聚的两嵌段聚合物——聚丙烯酸肉桂酸乙酯-b-(聚苯乙烯-r-聚丙烯酸叔丁酯),(记为PCEA-b-(PtBA-r-PS)).讨论了聚合过程中影响分子量分布以及分子量控制的各种因素.通过氢核磁(1H-NMR)确定各嵌段的重复单元数分别为50,111,138.通过透射电镜(TEM)观察,研究了该嵌段聚合物在选择性溶剂1-氯癸烷以及环戊烷中的自组装行为,发现该嵌段聚合物在环己烷中直接分散可以形成有聚集倾向的短棒状或球形胶束,而在1-氯癸烷中直接分散得到的胶束,在膜表面随着1-氯癸烷溶剂的缓慢挥发可以组装得到具有规则微纳结构的相互连接的柱状胶束.     

用减差红外光谱分峰法测定EVA共聚物的总支化度及支化度分布

对EVA大分子链上出现的支链结构,可选用无规聚丙烯的支链甲基峰1378cm~(-1),2-乙基己烷的支链乙基峰780cm~(-1)和聚α-己烯的支链丁基峰730cm~(-1)作为测定总支化度、乙基和丁基支化度的量度,并得到1000C中各支化度的分布公式:(L.B为长支链)n_3/1000C=0.50564 A_(1378)/dt-1.01966 n_(C_2H_5)/1000C=1.27161 A_(780)/dt-7.67873nC_(4H9)/1000C=0.09113 A_(730)/dt-6.41352 n_(L.B)/1000C=0.50564 A_(1378)/dt-1.27161 A_(780)/dt-0.09113 A_(730)/dt+13.07259由于EVA共聚物中,测定峰会发生重叠,故先用减差FTIR光谱分峰法,扣除干扰峰对测定峰的影响后,对测定峰进行峰面积积分,再计算支链的数均支化度,其测定结果与~1H-NMR结果一致。     

Polystyrene degradation induced by stresses resulting from the freezing of its solutions

Solutions of polystyrene in p-xylene were frozen in liquid nitrogen. No changes in molecular weight and distribution were caused by freezing solutions for a series of narrow distribution polystyrenes with molecular weights of near 2 × 10⁶ and lower. Likewise a commercial polystyrene of M?_w = 234,000 showed no change, even after 45 cycles of freezing and thawing. However, an ultrahigh molecular weight polystyrene (M?_w = 7.3 × 10⁶) showed appreciable degradation even after a few freezing cycles of its solutions. The changes in molecular weight and distribution were analyzed by gel-permeation chromatography. The results depended very much on the choice of solvent, cooling rate, and concentration. The extent of degradation was found to depend on polymer concentration in two distinct ways. Indeed, two different degradation mechanisms have been distinguished at low and at high concentrations. The change between mechanisms took place between 1.0 and 2.5 g/l. for polystyrene in p-xylene. This appears to provide a rare measure of polymer-polymer interactions (entanglements) in dilute solutions. Degradation in the entanglement region proceeded via a random chain-scission mechanism as tested by the Scott method. In contrast, at low concentrations degradation was characterized by the formation of appreciable amounts of low molecular weight polystyrene. The presence of an antioxidant (Ionol) during freezing did not change the extent of degradation significantly.     

平菇多糖稀溶液行为的研究

平菇多糖属生物高分子, 文章对平菇多糖稀溶液性质进行了研究。实验系采用Elias浊点滴定法测定平菇多糖溶液的θ组成, 用快速动态膜渗透计和粘度法测定平菇多糖的数均分子量、维利系数与分子链的构型参数。探讨其在θ条件下的分子形态及用Tung函数法等处理分级数据, 从而获得平菇多糖的分子量分布。     

Poly(2,6-diphenyl-1,4-phenyl oxide): Characterization by gel-permeation chromatography,light scattering,and solution viscosity

Ten unfractionated poly(2,6-diphenyl-1,4-phenylene oxide) samples were examined by gel permeation chromatography (GPC) and intrinsic viscosity [η] at 50°C in benzene, by intrinsic viscosity at 25°C in chloroform, and by light scattering at 30°C in chloroform. The GPC column was calibrated with ten narrow-distribution polystyrenes and styrene monomer to yield a “universal” relation of log ([η]M) versus elution volume. GPC-average molecular weights, defined as M?gpc = \documentclass{article}\pagestyle{empty}\begin{document}$\Sigma w_i [\eta ]_i M_i /\Sigma w_i [\eta ]_i$\end{document}, w_i denoting the weight fraction of polymer of molecular weight M_i, were computed from the GPC and [η] data on the polyethers. The M?GPC were then compared with the weight-average M?_w from light scattering. The intrinsic viscosity (dl/g) versus molecular weight relations for the unfractionated poly(2,6-diphenyl-1,4-phenylene oxides) determined over the molecular weight range 14,000 ≤ M?_w ≤ 1,145,000 are log [η] = ?3.494 + 0.609 log M?_w (chloroform, 25°C) and log [η] = ?3.705 + 0.638 log M?_w (benzene, 50°C). The M?_w(GPC)/M?_n(GPC) ratios for the polymers in the molecular weight range 14,000 ≤ M?_w ≤ 123,000 approximate 1.5 according to computer integrations of the GPC curves with the use of the “universal” calibration and the measured log [η] versus log M?_w relation. The higher molecular weight polymers (326,000 ≤ M?_w ≤ 1,145,000) show slightly broadened distributions.     

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.     

丁基锂引发聚合无规立构聚苯乙烯DSC曲线的比较研究

无规立构聚苯乙烯主链上不对称碳原子的构型是无规分布的，通常被认为是典型的非晶聚合物．一些研究者曾在热分析实验中发现从稀溶液中获得的无规立构聚苯乙烯样品ＤＳＣ扫描曲线Ｔｇ附近显现吸热峰，认为这些样品中存在某种局部有序区或准晶结构［１］．如何理解这种非晶...     

Living radical emulsion polymerization using the nanoprecipitation technique: An extension to atom transfer radical polymerization

Living radical polymerizations of styrene were performed under emulsion atom transfer radical polymerization conditions with latexes prepared by a nanoprecipitation technique recently developed for the stable free‐radical polymerization process. Latexes were prepared by the precipitation of a solution of low‐molecular‐weight polystyrene in acetone into a solution of a surfactant in water. The resulting particles were swollen with styrene and then heated. The effects of various surfactants and hydrophobic ligands, the reaction temperature, and the ligand/copper(I) bromide ratio were studied. The best results were obtained with the nonionic surfactant Brij 98 in combination with the hydrophobic ligand N,N‐bis(2‐pyridylmethyl)octadecylamine and a ligand/copper(I) bromide ratio of 1.5 at a reaction temperature of 85–90 °C. Under these conditions, latexes with good colloidal stability with average particle diameters of 200 nm were obtained. The molecular weight distributions of the polystyrenes were narrow, although the experimental molecular weights were slightly larger than the theoretical ones because not all the macroinitiator appeared to reinitiate. © 2006 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 44: 4027–4038, 2006     

The hexagonal phase and melt of low-molecular-weight polyethylene

Phase diagrams of low-molecular-weight polyethylene (M = 1000, 2000, 6500, 16,000) and polyethylene (M ≈ 1,000) after fuming nitric acid treatment have been determined from 20 to 300°C up to pressures of about 10 kbar. The fractions with molecular weights 1000 and 2000 do not exhibit the hexagonal phase, but the others do. Effects of molecular weight and fuming nitric acid treatment on the phase diagrams are discussed in terms of the entropy of the melt.     

Tuning the hemolytic and antibacterial activities of amphiphilic polynorbornene derivatives

Amphiphilic cationic polynorbornene derivatives, soluble in water, were prepared from modular norbornene monomers, with a wide range of molecular weights (M(n) = 1600-137 500 g/mol) and narrow polydispersities (PDI = 1.1-1.3). The antibacterial activity determined by growth inhibition assays and the hemolytic activity against human red blood cells were measured and compared to determine the selectivity of the polymers for bacterial over mammalian cells. The effects of monomer repeat unit hydrophobicity and polymer molecular weight on antibacterial and hemolytic activities were determined. The hydrophobicity of the repeat unit was observed to have dramatic effects on antibacterial and hemolytic activities. Lipid membrane disruption activities of the polymers was confirmed by measuring polymer-induced dye leakage from large unilamellar vesicles. By tuning the overall hydrophobicity of the polymer through random copolymerizations of modular norbornene derivatives, highly selective, nonhemolytic antibacterial activities were obtained. For appropriate monomer composition, selectivity against bacteria versus human red blood cells was determined to be over 100.     

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。     

Kinetics of the adsorption of polystyrene macromolecules from dilute solutions in methyl ethyl ketone on carbon black

The kinetics of the adsorption of a mixture of three polystyrenes (the weight-average molecular weight M _w = 8300, 34000, and 195000) on nonporous carbon (carbon black pretreated in the argon flow at 3800 K) from dilute solutions in methyl ethyl ketone at 298 K is studied. The kinetic dependences of the adsorption of polystyrenes on carbon black nanoparticles from solutions in methyl ethyl ketone are described by adsorption kinetics equations previously used for describing the adsorption of aromatic hydrocarbons from aqueous solutions by active carbon. The correlation between the kinetic coefficients and the molecular weights of polystyrenes is discussed.