关于高分子极稀溶液粘度测定问题的探讨

对聚苯乙烯(PS)／甲苯稀及极稀溶液的粘度用常规的乌氏粘度法进行了测定．发现高分子在毛细管壁上无稳固吸附．在极稀浓度区，粘数(ηsp/c)值波动较大，在时间测量精度不变的条件下，粘数测量误差与浓度成反比，以致ηsp／c-c曲线的线性及重现性变差，并推导出了粘数测量误差与浓度及时间测量误差间的关系式．在此基础上，讨论了确定浓度测量下限的原则及计算公式，认为常规的乌氏粘度测定方法对极稀溶液的应用值得商榷．     

真空浇铸聚苯乙烯薄膜的拉伸力学行为

高分子溶液的浓度从极稀到极浓的转变过程是高分子链从单链体系转变成相互穿透的多链体系的分子凝聚过程 .在极稀溶液中高分子链以无规线团状态孤立地存在于溶剂介质中 ;在良溶剂中是溶涨的无规线团 ,可以设想溶液浓度逐渐增大时 ,有一高分子线团开始相互接触的所谓接触浓度 ;随着浓度进一步增加高分子线团之间就发生交叠而相互穿透 ,这时溶液就转变成物理交联结构的浓溶液 .分子链的互穿程度会随浓度的继续增加而增加 .如果能用一些特殊的实验方法将高分子在不同浓度的溶液中的凝聚状态尽量全部或部分的保留到高分子固体中 ,则所得到的具有…     

大分子溶致凝聚过程中的几个分界浓度

按照现代高分子凝聚态物理学观点,高分子溶液按浓度分为:极稀溶液、稀溶液、亚浓溶液、浓溶液、极浓溶液5个层次,各层次间的分界浓度分别称为动态接触浓度、接触浓度、缠结浓度和全高斯链浓度,其中全高斯链浓度由本文作者命名。文中给出各分界浓度的定义,介绍各分界浓度的物理意义,特别说明命名全高斯链浓度的依据。同时详细讨论了不同浓度溶液中大分子链的构象及其变化、链间相互作用的本质和微观图像、以及溶液浓度变化对溶液性质的影响。     

多分散高分子的稀溶液粘度-浓度依赖性

依据最近提出的关于单分散高分子的稀溶液粘度的团簇理论,对多分散高分子的稀溶液粘度的浓度依赖性进行了更新的理论分析。最后得到一个新的多分散高分子的稀溶液粘度与浓度的关系式。实验研究表明,该关系式是与实验数据相一致的。     

聚电解质溶液浓度区域的划分

按照De Gennes提出的标度概念,柔性高分子溶液可以划分为稀溶液,亚浓溶液和浓溶液3个区域,它们之间分别以接触浓度C^**和交叠浓度C^**为分界线．钱人元等根据聚苯乙烯溶液激基荧光强度浓度依赖性的实验结果,提出稀溶液区还应细分为极稀溶液和稀溶液两个区域,它的分     

高分子混合物溶液在极稀浓度区的粘度异常行为

上世纪50年代初人们就发现,高分子溶液的粘度在极稀浓度区往往表现出异常行为,即当浓度低于某一特定值后,比浓增比粘度-浓度图偏离预计的线性关系,出现上弯或下弯的曲线.     

聚乙烯醇水溶液反复冷冻过程中的溶剂化效应

采用示差扫描量热技术(DSC)对聚乙烯醇(PVA)水溶液反复冰冻过程中的溶剂化效应进行研究.引入水化数的概念来表征溶剂化效应的大小.结果表明不同浓度区间的PVA水溶液其在反复冰冻过程中溶剂化效应显著不同,主要归因于高分子链分子内和分子间缠结程度对溶剂分子"参与"溶剂化的程度和方式的不同.作者把极稀高分子溶液的研究结果拓展到高分子稀溶液或亚浓溶液区间,阐述了高分子溶液中高分子链的物理图像.冷冻次数的增加导致链间缠结增加,部分溶剂则被包裹在由链间缠结点所形成的网圈内成为分子链的一部分.溶液溶剂化程度的变化受到包裹溶剂与高分子链脱溶剂化的综合影响.     

关于极稀或极弱碱溶液pOH值的计算问题

对于浓度不是很稀,碱性不是很弱的碱溶液,计算溶液中OH-的浓度时,往往忽略了水的离解的影响,采用近似计算公式求得OH-的近似浓度。这在许多情况下是可以的,且计算结果亦比较满意。但是对于极稀或极弱碱溶液能否采用近似公式计算呢?如果不能的话,应该采用怎样的计算公式才能得到比较满意的结果呢?下面举二例予以说明。一、极稀极弱碱溶液对于极稀极弱碱溶液,由于溶液中OH-的浓度非常小,所以就不能忽略水本身离解出来的OH-,甚至它可能就是OH-的主要来源。     

支化高分子稀溶液粘度的浓度依赖性

自缔合平衡常数;支化高分子稀溶液粘度的浓度依赖性     

脱氧核糖核酸分子在高分子溶液3个不同浓度区间的电泳迁移行为

 借鉴高分子亚浓溶液线团收缩理论 ,研究了脱氧核糖核酸 (DNA)片段在高分子溶液全浓度区间的电泳迁移行为。结果表明 ,在高分子稀溶液、亚浓溶液和浓溶液 3个不同浓度区间 ,DNA的电泳迁移行为各不同 ,DNA片段的分离在这 3个浓度区间也存在差异。     

Diffusion-controlled growth of lamellar crystals in an isotactic polystyrene–polyphenylene oxide blend

The growth rates of lamellar crystals grown onto preseeded fibrillar crystals (“shishes”) in isotactic polystyrene and blends of isotactic polystyrene (iPS) with polyphenylene oxide are followed by using transmission electron microscopy. The preseeded fibrillar crystals avoid the problem of timedependent primary nucleation. The time dependence of lamellar growth is investigated. At a concentration of 50% PPO in iPS, the lateral lamellar growth rate of the precipitating isotactic polystyrene crystals conforms to a time law characteristic of diffusion-controlled growth (R ∝ t^1/2). Diffusion coefficients are estimated from the growth kinetics. The method could prove a simple means of measuring diffusion coefficients in polymer blends in which one component is crystallizable.     

单链和寡链等规聚苯乙烯聚集体的结晶行为

自1960年Hoffman等提出聚合物结晶成核理论以来,人们对聚合物结晶生长速率、片晶的侧向尺寸随过冷度的变化等现象成功地进行了理论描述．1997年,Hoffman等对聚合物结晶成核理论进行修正,将de Gennes的聚合物“蛇行”概念。引入表面成核理论,通过对单根分子链从过冷熔体“卷绕”到晶体前沿所需的时间进行估算,其结果远远低于Flory预言时间约3～5个数量级,据此,Hoff-man认为,在聚合物结晶过程中,分子链在强迫稳态下的“蛇行”运动有足够的时间解缠结和结晶。     

Determination and Temperature Dependence of Plateau Modulus for Polymerization of Propylene to Isotactic Polypropylene with Ultra-high Molecular Weight under Catalysis of Ziegler-Natta Catalyst

The viscoelastic behavior of isotactic polypropylene with ultra-high molecular weight (UHPPH) and broad molecular weight distribution(MWD), produced in the presence of Ziegler-Natta catalyst, was investigated by means of oscillatory rheometry at 180 and 200 ℃, whose loss modulus(G") plots at 180 and 200 ℃versus the natural logarithm of angular frequency(ω) present a pronounced maximum at 34.35 and 69.21 rad/s, respectively, and do not show a maximum peak at 0. 01-100 rad/s for Ziegler-Natta catalyzing ethylenepropylene random copolymerization (PPR) with a conventional molecular weight and broad MWD. The fact indicates that the high molecular weight is responsible for a maximum peak of G"(ω) vs. lnω curves for UHPPH. This makes it possible to determine the plateau modulus (G0N) of UHPPH from a certain experimental temperature G"(ω) curve directly. For UHPPH, the G0N determined to be 4. 28×105 and 3. 62×105 Pa at 180and 200 ℃, respectively, decreases with the increase of temperature and is independent of the molecular weight, which directly confirms reputation theoretical prediction that the G0N has no relation to the molecular weight.     

Four organic crystals displaying distinctively different emission colors based on an ESIPT-active organic molecule

Multi-colored fluorescence which covering pure K^* emission, E^*&K^* emission and pure E^* emission was obtained by controlling the preparation conditions of a simple ESIPT-active molecule.     

Single-chain single crystals

Single-chain single crystals of isotactic polystyrene and poly(ethylene oxide) were studied by using transmission electron microscopy, high resolution electron microscopy, electron diffraction. Single-chain single crystals were prepared by spreading a dilute solution of polymers on a water surface and collecting the resulting single-chain particles on copper grids, followed by isothermal crystallization. A statistical analysis of the sizes of single-chain crystals was found to match with the known molecular weight distribution of original sample, indicating the particles to be composed of single chain. Observation of the morphology and electron diffraction gave evidence of the single crystal nature. Regular-shaped single-chain crystals were obtained after isothermal crystallization for a longer time. By close observation, several types of morphologies were found for single-chain crystals of isotactic polystyrene and poly(ethylene oxide); in addition to the conventional morphologies observed for multi-chain crystals, new morphologies were observed in both cases. The morphologies of poly(ethylene oxide) were explained according to the crystal structure and twin modes. Tent-like single-chain crystals were often observed. Because of the small size of the crystals, they can avoid collapse on the substrate. The crystalline c-axis of single-chain crystals were found to orient preferably in the direction normal to the substrate. The investigation of electron diffraction and high resolution electron microscopy revealed that the structure of the single-chain crystals of isotactic polystyrene is the same as for multi-chain crystals. A reasonable explanation is given for the unusual resistance to electron irradiation and the missing of lower-index reflections. Regular periodic stripes were found on the top surface of single-chain crystal of isotactic polystyrene with an average periodic length in accordance with (220) spacing. In addition, a statistical thermodynamics theory was developed for single-chain crystal. It is found that the equilibrium dimensions are related to molecular weight and annealing temperature, while the equilibrium melting temperature depends on molecular weight.     

Polymer crystallization: Simulation with entropic barrier model and application to specific polymers

The growth of polymer single crystals has been simulated on the basis of a simple two-dimensional ‘entropic barrier’ model. The chain is described by a sequence of growth units. Their additions and removals are determined by rate constants obeying detailed balance. The crystallization is then simulated by a kinetic Monte Carlo algorithm. An application of the model to specific crystallizable polymers (polyethylene, isotactic polystyrene, isotactic polypropylene, polyhydroxybuterate and polypivalolactone) is presented. Input parameter values for the model are derived from the respective surface free energies, bulk enthalpies, melting points and crystallographic repeat lengths. The only free parameter is the length of a polymer growth unit. This is set to half the lamellar crystal thickness at large undercooling. The lamellar thicknesses calculated on this basis are in good agreement with experimental data. An analysis of the growth unit lengths of the different polymers indicates a scaling with the chain persistence length in the melt.     

On the lateral size of shish crystals

The lateral sizes of shish crystals crystallized from high-molecular-weight isotactic polystyrene and different blends with atactic polystyrene were examined with the help of transmission electron microscopy. It is found that the lateral sizes of shish crystals decrease with increasing content of the noncrystallizable aPS. A model accounting for the observation is proposed.     

MFI型分子筛膜的两段变温合成及对二甲苯异构体的分离性能

分别采用恒温和变温两种方法在氧化铝支撑体上原位制备了MFI型分子筛膜. 恒温法合成的MFI型分子筛膜晶体颗粒较大, 在高温脱除模板剂时会形成较大的缺陷, 没有对二甲苯/邻二甲苯(PX/OX)分离性能. 变温法合成的MFI型分子筛膜晶体在a, b方向尺寸较小, 在高温脱除模板时不会形成较大缺陷, 对PX/OX有良好的分离性能, 在300 ℃下, PX/OX分离因子高达42, PX的渗透性为9.57×10^-9 mol·m^-2·s^-1·Pa^-1. 采用低温臭氧脱除模板剂能够有效减小分子筛晶体热收缩产生的应力, 提高MFI型分子筛膜的分离性能. 两种方法合成的分子筛膜在低温臭氧的条件下脱除模板剂后, 都具有PX/OX分离性能, 其中变温法合成的分子筛膜PX/OX分离因子高达76, PX的渗透性为1.02×10^-8 mol·m^-2·s^-1·Pa^-1.     

Gelation-crystallization in isotactic polystyrene solutions and its implications to crystal morphology,to the origin and structure of gels,and to the chemical homogeneity of polyolefins

As part of a wider study on the crystallization of isotactic polystyrene solutions it was observed that at sufficient concentrations (> 3–5%) gelation sets in below a certain (very high) supercooling in competition with the usual single crystal formation which in itself produces turbid suspensions. It was established that gelation is a form of crystallization (mode A) which must be of fringed micellar type to provide the connectedness as opposed to the chain folded lamellae (mode B) which gives rise to discrete particles. The gel crystals (A) display sharp melt endotherms and produce distinct x-ray diffraction patterns both of which, however, differ decisively from those provided by crystals B, a distinction which can be preserved even after removal of the solvent. The melting points of A are significantly lower than those of B and the x-ray diffraction patterns of A are incompatible with the recognized structure of polystyrene (3₁ helix) possessed by B; they point to a broadly planar zig-zag arrangement of the chain. This strongly suggests that we have blocks of chemically distinct sequences which could be syndiotactic or head-to-head tail-to-tail (presently with substantial support for the latter) which is responsible for the gel forming crystallization. However, so far the C¹³ nuclear magnetic resonance (NMR) results do not provide the evidence for these distinct species but explanations for our observations on any other basis seem to lead to unsuperable difficulties from other points of view. Consequently, the paper is left open ended with the possibilities discussed. Amongst these the existence of a very few but long, chemically distinct sequences seems most attractive. The wider implications of the facts as they stand for crystal morphology (fringed micelles versus lamellae), for the origin and structure of gels in general, for the crystallization of block copolymers and for issues relating to chemical homogeneity (tacticity, head-to-head tail-to-tail) are discussed and preliminary effects are quoted which indicate that these issues may also be relevant to the usual atactic polymers.     

粘度法和超离心沉降法测定环型聚苯乙烯分子量

本文介绍了测定环型聚苯乙烯分子量的两个计算关系式。