羧化聚苯醚与聚苯乙烯共混体系相分离初期分子量影响的光散射研究

本文用激光光散射方法研究了具有特殊相行为[(低临界溶解温度(LCST),高临界溶解温度(UCST)共存]共混体系羧化聚苯醚和聚苯乙烯在UCST域内的不稳相分离初期分子量对动力学参数的影响。结果表明:相分离初期动力学过程与Cahn理论吻合;随着分子量增加,表现扩散系数D_(a??)明显减小;该体系的表现扩散系数为10~(-14) cm~2s~(-1)数量级。deGennes管子模型可很好地描述不稳相分离初期大分子扩散行为。     

羧化聚苯醚与聚苯乙烯共混体系相分离初期分子量影响的光散射研究

 本文用激光光散射方法研究了具有特殊相行为[(低临界溶解温度(LCST),高临界溶解温度(UCST)共存]共混体系羧化聚苯醚和聚苯乙烯在UCST域内的不稳相分离初期分子量对动力学参数的影响。结果表明:相分离初期动力学过程与Cahn理论吻合;随着分子量增加,表现扩散系数D_app明显减小;该体系的表现扩散系数为10^-14 cm²s^-1数量级。deGennes管子模型可很好地描述不稳相分离初期大分子扩散行为。     

聚甲基丙烯酸甲酯与苯乙烯-丙烯腈共聚物混合体系相分离初期的固体NMR研究

本文用氢谱宽线固体NMR技术研究了聚甲基丙烯酸甲酯(PMMA)和苯乙烯-丙烯腈共聚物(SAN)混合体系不稳相分离初期阶段, 得到了在分相过程中弛豫谱的变化规律, 测定了相分离增长速率。结果指出: 随着退火时间的增加, 两相体系形成; 大分子扩散方式是由浓度低的区域向浓度高的区域扩散, 扩散系数为负值; 相分离增长速率的数量级与用光散射研究的结果相同; 分子相互作用的相关距离为46.5 nm。     

聚甲基丙烯酸甲酯与苯乙烯-丙烯腈共聚物混合体系相分离初期的固体NMR研究

本文用氢谱宽线固体NMR技术研究了聚甲基丙烯酸甲酯(PMMA)和苯乙烯-丙烯腈共聚物(SAN)混合体系不稳相分离初期阶段,得到了在分相过程中弛豫谱的变化规律,测定了相分离增长速率。结果指出:随着退火时间的增加,两相体系形成;大分子扩散方式是由浓度低的区域向浓度高的区域扩散,扩散系数为负值;相分离增长速率的数量级与用光散射研究的结果相同;分子相互作用的相关距离为46.5nm。     

PMMA/SAN共混体系相分离的固体NMR研究

本文用~1H谱宽线固体NMR技术研究了聚甲基丙烯酸甲酯(PMMA)和苯乙烯—丙烯腈共聚物(SAN)共混体系不稳相分离初期过程,得到了在相分离过程中弛豫谱的变化规律,测定了相分离增长速率。结果表明,随着淬火时间的增加,两相体系形成,大分子扩散方式是由浓度低的区域向浓度高的区域扩散,扩散系数为负值;相分离增长速率的数量级与用光散射研究的结果相同;分子相互作用的相关距离为46.5nm。     

聚甲基丙烯酸甲酯/聚醋酸乙烯酯共混分相过程结构函数的标度分析和相凝聚

高分子共混体系相分离动力学研究已取得了很大的进展。Cahn理论可很好地描述相分离初期过程,de Gennes的蛇行理论可较好地描述相分离初期大分子扩散。在相分离后期,人们已经发现动力学参量的标度行为,但实验结果不一,标度成因尚不十分清楚。本文研究了聚甲基丙烯酸甲酯(PMMA)/聚醋酸乙烯酯(PVAc)共混体系相分离后期过程。分析了结构函数的标度行为,初步讨论了相凝聚特征。     

不同热塑性树脂改性热固性树脂体系反应诱导相分离过程的时间/温度依赖性

对几种不同热塑性树脂改性热固性树脂体系反应诱导相分离过程,包括UCST(最高互溶温度)、LCST(最低互溶温度)体系和含有复杂多步反应体系,在耐高温高分辨热台显微镜、流变仪和小角激光光散射仪上进行了研究.发现体系的反应诱导相分离时间/温度关系遵循Arrhenius方程.其相分离活化能对体系反应速率、粘弹性变化、体系中热塑性树脂的含量和分子量不敏感,也不受相分离检测手段的影响,而依赖于树脂化学环境相容性和交联反应的温度依赖性.对这一共性的物理本质进行了讨论.     

等规聚丙烯/二元乙丙橡胶合金相分离对结晶动力学的影响

用小角激光光散射(SALLS)、相差显微镜(PCM)、示差扫描量热仪(DSC)和偏光显微镜(POM)研究了聚丙烯/二元乙丙橡胶(iPP/EPR)共混体系的相分离行为和等温结晶行为.发现iPP/EPR(50/50,W/W)发生的液-液相分离遵循spinodal机理.通过Cahn-Hilliard方程求得了不同实验温度下iPP/EPR的表观扩散系数(Dapp)以及spinodal温度(Ts).考察了不同相分离程度的iPP/EPR体系结晶动力学,发现延长相分离时间(tps)或提高相分离温度(Tps)均会导致半结晶时间(t1/2)增大,即结晶速率降低.这被归于EPR成核作用的降低.动力学分析结果表明Avrami模型适用于描述该体系的等温结晶过程,其结晶机理基本不受相分离程度的影响,结晶均以瞬时成核和三维生长为主.     

一些热塑改性热固性树脂体系结构对反应诱导相分离时间/温度依赖性的影响

利用光学显微镜、DSC等手段研究了一些上临界共溶温度(UCST)类型的热塑性改性热固性树脂体系反应诱导相分离时间/温度依赖性随组分化学结构的变化规律.结果表明,分相活化能Ea(ps)受热塑性树脂的主链结构、热固性单体、交联剂结构、化学计量比等因素的影响.利用相互作用能密度解释了实验所研究的UCST体系的相分离活化能Ea(ps)随组分结构的变化规律.     

聚甲基丙烯酸甲酯/(苯乙烯-丙烯腈)共聚物混合体系的早期分离

本文用激光光散射技术研究了高分子混合体系聚甲基丙烯酸甲酯/(苯乙烯-丙烯腈)共聚物(PMMA/PSAN)不稳相分离(Spinodal decomposition)过程,结果指出,相分离前期符合Cahn理论预言的结果;首次用光散射技术在高分子混合体系相分离研究中得到了不稳相分离增长速率最大值R(q_m);只(q)的实验结果与理论值相吻合;证实了界面自由能对相分离增长速率的影响是不可忽略的。     

Relaxation processes in mixtures of liquid crystals and polymers near phase boundaries and during phase separation

We present experimental studies of the relaxation of concentration fluctuations in a semidilute solution of polystyrene (PS) (30% by weight) in 4-cyano-4'-n-octyl-biphenyl (8CB) (70% by weight) using the photon correlation spectroscopy (PCS). In the homogeneous phase there are two modes of relaxation. The slow one (typical time scale is taus = 0.001 s) is due to the diffusion of polymer chains (of molecular mass 65,000) in the LC matrix (of molecular mass 290), while the fast one has the time scale of the order of tauf approximately 0.00001 s. The amplitude of the fast mode is much weaker than the one for the slow mode. Moreover it does not depend on the scattering wave vector, q. The value of the diffusion coefficient, Dc = 1/(tausq2) for the slow mode decreases with temperature according to the Arhenius law until we reach the coexistence curve. Its value close to the coexistence is Dc = 4 x 10(5) nm2/s and the activation energy in the homogeneous mixture is Ec=127 kJ/mol. If we gradually undercool the mixture below the coexistence into the metastable two-phase region without inducing the phase separation we find unexpectedly that Dc does not change with temperature even 4 degrees below the coexistence curve. The characteristic time of the fast mode does not depend on the scattering wave vector indicating that it is related to the transient gel structure. We have shown that it is possible to measure the short time relaxation of concentration fluctuations during the phase separation in the mixture. At low temperature close to the isotropic-nematic phase transition we have observed that the relaxation is well separated in time from the typical time of the domain growth. This relaxation mode is characterized by the large diffusion coefficient D = 2 x 10(8) nm2/s. The mode probably comes from the coupling between the orientational dynamics of liquid crystals and the transient gel structure of polymers.     

Determination of the interconversion energy barrier of 2,3-pentadienedioic acid enantiomers by HPLC. 2. On-column interconversion

In this paper, an HPLC method is used to determine the enantiomerization barrier of 2,3-pentadienedioic acid enantiomers. The racemate of 2,3-pentadienedioic acid was separated by HPLC on a chiral CHIROBIOTIC T column with a 90:10 (100:0.5:0.5 MeOH/HOAc/TEA)/H2O mobile phase. Peak areas of enantiomers prior to (A(+)0, A(-)0) and after the separation (A(+), A(-)), were used for calculation of the rate constants and the enantiomerization barrier, as determined by computer-assisted peak deconvolution of the peak clusters on the chromatograms. The kinetic equation for irreversible reactions was used to determine the apparent enantiomerization rate constants and the interconversion energy barrier. The dependence of the apparent enantiomerization barrier (deltaG1(app), deltaG-1(app)) on temperature was used to determine the apparent activation enthalpy (deltaH1(app), deltaH(-1)app) and entropy (deltaS1(app), deltaS-1(app)) for the interconversion of 2,3-pentadienedioic acid enantiomers, where the coefficients 1 and -1 designate the interconversions (+) --> (-) and (-) --> (+), respectively.     

海藻酸钠-壳聚糖-粉末活性炭生物微胶囊的传递性能研究

测定不同分子量的聚乙二醇(PEG)溶液透过海藻酸钠-壳聚糖-粉末活性炭(SA-CA-PAC)生物微胶囊的性能,确定了SA-CA-PAC膜的截留分子量在PEG4000以下。研究了葡萄糖、乳糖、氨基酸等小分子的物质在SA-CA-PAC微胶囊中的扩散性能,用数学模型计算出了这些物质在微胶囊的混合扩散系数Dm以及相应的微胶囊膜层中扩散系数D1,结果表明小分子量的物质具有较好的扩散性能,且Dl<相似文献   

Gas chromatographic determination of the interconversion energy barrier for dialkyl 2,3-pentadienedioate enantiomers

The enantiomers of dialkyl 2,3-pentadienedioate undergo interconversion during gas chromatographic separation on chiral stationary phases. In this paper the on-column apparent interconversion kinetic and thermodynamic activation data were determined for dimethyl, diethyl, propylbutyl and dibutyl 2,3-pentadienedioate enantiomers by gas chromatographic separation of the racemic mixtures on a capillary column containing a polydimethylsiloxane stationary phase coupled to 2,3-di-O-methyl-6-O-tertbutyldimethylsilyl-beta-cyclodextrin. A deconvolution method was used to determine the individual enantiomer peak areas and retention times that are needed to calculate the interconversion rate constants and the energy barriers. The apparent rate constants and interconversion energy barriers decrease slightly with an increase in the alkyl chain length of the dialkyl 2,3-pentadienedioate esters. The optimum conformation of the dialkyl 2,3-pentadienedioate molecules, their separation selectivity factors and apparent interconversion enthalpy and entropy data changes with the alkyl chain length. The dependence of the apparent interconversion energy barrier (deltaG(app)(a-->b), deltaG(app)(b-->a)) on temperature was used to determine the apparent activation enthalpy (deltaH(app)(a-->b), deltaH(app)(b-->a)) and apparent entropy (deltaS(app)(a-->b), deltaS(app)(a-->b)) (where a denotes the first and b second eluted enantiomer). The comparison of the activation enthalpy and entropy (deltaS(app)(a-->b), deltaS(app)(a-->b)) indicated that the interconversion of dialkyl 2,3-pentadienedioate enantiomers on the HP-5+Chiraldex B-DM column series is an entropy driven process at 160 degrees C. Data obtained for dimethyl 2,3-pentadienedioate enantiomers on the HP-5+Chiraldex B-DM column series at 120 degrees C (deltaG(app)(a-->b) = 123.3 and deltaG(app)(b-->a) = 124.4 kJ mol(-1)) corresponds (at the 95% confidence interval) with the value of deltaG(#) = 128+/-1 kJ mol(-1) found at this temperature by gas chromatography using a two-dimensional stop flow technique on an empty capillary column [V. Schurig, F. Keller, S. Reich, M. Fluck, Tetrahedron: Asymmetry 8 (1997) 3475].     

Transport properties of solid polymer electrolytes prepared from oligomeric fluorosulfonimide lithium salts dissolved in high molecular weight poly(ethylene oxide)

Transport properties such as ionic conductivity, lithium transference number, and apparent salt diffusion coefficient are reported for solid polymer electrolytes (SPEs) prepared using several oligomeric bis[(perfluoroalkyl)sulfonyl]imide (fluorosulfonimide) lithium salts dissolved in high molecular weight poly(ethylene oxide) (PEO). The salt series consists of polyanions in which two discrete fluorosulfonimide anions are linked together by [(perfluorobutylene)disulfonyl]imide linker chains. The restricted diffusion technique was used to measure the apparent salt diffusion coefficients in SPEs, and cationic transference numbers were determined using both potentiostatic polarization and electrochemical impedance spectroscopy methods. A general trend of diminished salt diffusion coefficient with increasing anion size was observed and is opposite to the trend observed in ionic conductivity. This unexpected finding is rationalized in terms of the cumulative effects of charge carrier concentration, anion mobility, ion pairing, host plasticization by the anions, and salt phase segregation on the conductivity.     

Entanglement and phase separation in hyperbranched polymer/linear polymer/solvent ternary blends

Hyperbranched polyethylene (HBPE)/linear polystyrene (PS)/chloroform (CF) solution was selected as a model system to investigate the effect of branching structure on entanglement and phase separation behavior in semi-dilute ternary polymer solutions. All the HBPE materials in this work were found to have similar chain architectures and the critical molecular weight was estimated to be 81.2 kDa. The results obtained by elastic light scattering and intrinsic fluorescence methods suggested that all ternary solutions exhibited UCST transition behavior upon cooling. Also, it was found that the increase in the molecular weight of PS led to increase in the phase separation rate, consistent with de Gennes prediction. However, the increase of molecular weight of HBPE did not monotonously reduce the compatibility of polymer components and the phase separation rate in ternary blends is as follows: medium molecular weight HBPE (HBPE-M) > high molecular weight HBPE (HBPE-H) > low molecular weight HBPE (HBPE-L). This abnormal behavior can be explained by the fact that, (i) for HBPE-L, no entanglements between HBPE chains occurred and the branching effect can be ignored, and (ii) for HBPE-M and HBPE-H, entanglement of HBPE chains can be formed, and the dilution of branches on entanglement of backbones should be taken into consideration, that is, the shorter the branches of HBPE, the higher the possibility of interpenetration of HBPE backbones between neighboring molecules and, consequently, the faster aggregation of HBPE during phase separation. Furthermore, a simple model based on decomposition reaction was proposed to quantitatively describe the phase separation kinetics and the apparent activation energies of phase separation were calculated to be −150.3 and −52.3 kJ/mol for HBPE-M/PS/CF and HBPE-H/PS/CF systems, respectively.     

聚丙烯酸凝胶的动态行为及温敏相变

应用动态光散射技术研究了聚丙烯酸凝胶的动态行为及温敏相变．以相关长度（ξ）及扩散系数（Ｄ）表征动态行为．交联度,聚合物浓度及引发剂用量对ξ和Ｄ影响的规律是,随交联度增加,ξ和Ｄ分别减小及增大;聚合物浓度高,扩散系数大;引发剂用量增大,ξ向变小的方向发展．温敏相变的规律是,随温度升高,Ｄ增加,ξ下降,并且ξ分布范围逐渐变窄;随温度下降,因χ 诱发的微脱水收缩作用而导致相分离,出现浊度;交联度愈高,出现相分离的温度愈高．