高分子三重态敏化剂的研究IV: 高分子苯乙酮及其衍生物的光谱, 磷光量子产率及光敏化光稳定问题的研究

本工作合成和研究了高分子苯乙酮及其衍生物的光谱、磷光量子产率、磷光寿命以及光敏化、光稳定等问题。结量表明高分子光敏化剂和光稳定剂保持着它们原来相应小分子的光化学和光物理行为。高分子敏化剂由于T-T湮灭, 分子链中的光敏基团的存在一最佳值, 此时磷光量子产率最高, 敏化效率最好。但高分子光稳定剂则光稳定基团含量愈高光稳定能力愈强。     

高分子三重态敏化剂的研究——Ⅳ.高分子苯乙酮及其衍生物的光谱、磷光量子产率及光敏化光稳定问题的研究

本工作合成和研究了高分子苯乙酮及其衍生物的光谱、磷光量子产率、磷光寿命以及光敏化、光稳定等问题.结果表明高分子光敏化剂和光稳定剂保持着它们原来相应小分子的光化学和光物理行为.高分子敏化剂由于T-T湮灭,分子链中的光敏基团的含量存在一最佳值,此时磷光量子产率最高,敏化效率最好.但高分子光稳定剂则光稳定基团含量愈高光稳定能力愈强.     

高分子光稳定剂的研究——溶解度参数与光稳定效率的关系

<正> 添加光稳定剂是阻止聚合物因光照氧化降解,延长聚合物制品的使用寿命的有效方法。显然只有当光稳定剂能最大程度地均匀分散在聚合物中才能充分地发挥它的光稳定效率,这对高分子光稳定剂来说尤为重要。 光稳定剂与被稳定的聚合物的相容性对光稳定效率的影响已有过研究。如Ambrovic等曾经报道:随着2-羟基4-烷氧基二苯甲酮中烷基的碳原子数增加,它对聚丙烯的光稳定效率提高。高分子光稳定剂本身是一个有一定分子量的聚合物,使用时它与被稳定聚合物形成了共混体系。我们研究了高分子光稳定剂的溶解度参数和它对聚丙烯的光稳定效率的关系。     

一类新型三线态敏化剂光物理行为的研究

本文对一类新型的三线态敏化剂N-甲基芳酰基甲基-β-萘骈噻唑啉的光物理行为进行了研究。测定了它们的吸收光谱、荧光和燐光量子产率。发现所研究的敏化剂比常用敏化剂有着较高的克分子吸收系数(～10~4),还具有较高的系间窜跃能力。本文还测定了存在不同敏化剂时,芪的顺、反异构化反应速度,以此评价化合物的敏化效率。认为这类化合物是有效的新型光敏化剂。     

某些高分子受阻胺对聚丙烯稳定化作用的研究

众所周知,受阻胺光稳定剂对聚烯烃有良好的光稳定效率,已引起世界的注意。然而,小分子量的受阻胺易于挥发,从而影响它的效率发挥^[1,2],为了克服这个缺点,使小分子受阻胺的高分子化是近年来受阻胺光稳定剂发展的方向,本文主要是研究三种商品化高分子受阻胺光稳定剂对聚丙烯的稳定化作用及其效率和机理。     

高分子三重态敏化剂的研究III: 高分子苯乙酮敏化过程中能量迁移的研究

本工作合成了一组不同组成的聚(苯乙烯-乙烯基苯乙酮)高分子敏化剂, 对分子中两组分的含量进行了标定. 通过荧光和磷光光谱的研究表明: 高分子敏化剂分子中存在着单重态和三重态的能量迁移和T-T湮灭作用.从降冰片二烯光敏异构化为四环烷的反应中发现, 苯乙酮摩尔含量为38%的高分子苯乙酮敏化剂具有最大的敏化能力, 并对上述诸现象产生的原因进行了分析和讨论.     

高分子三重态敏化剂的研究 Ⅲ.高分子苯乙酮敏化过程中能量迁移的研究

本工作合成了一组不同组成的聚(苯乙烯-乙烯基苯乙酮)高分子敏化剂,对分子中两组分的含量进行了标定.通过荧光和磷光光谱的研究表明:高分子敏化剂分子中存在着单重态和三重态的能量迁移和 T~*-T~ 湮灭作用.从降冰片二烯光敏异构化为四环烷的反应中发现,苯乙酮摩尔含量为38％的高分子苯乙酮敏化剂具有最大的敏化能力,并对上述诸现象产生的原因进行了分析和讨论.     

衍生化高效液相色谱法测定高分子受阻胺光稳定剂

以对硝基苯甲酰氯为酰基化试剂,通过与含胺基的高分子受阻胺光稳定剂944在四氢呋喃中发生酰胺化反应形成沉淀,改变反应配比确定对硝基苯甲酰氯与高分子受阻胺光稳定剂944反应比例为5∶1。利用傅立叶红外光谱分析反应沉淀来实现高分子受阻胺光稳定剂944的定性分析,利用高效液相色谱分析反应上层清液,实现定量分析,紫外可见检测器检测波长为360 nm,反应测试结果回收率可达到90%以上。     

高分子受阻胺对顺1,4-聚丁二烯溶液光敏降解过程的稳定作用

本文研究了高分子受阻胺光稳定剂苯乙烯4-(甲基丙烯酸)-2,2,6,6-四甲基哌啶醇酯共聚物在用罗丹明6G光敏氧化降解顺1,4-聚丁二烯过程中的稳定作用。它具有淬灭单线态氧、分解过氧化氢以及捕获大分子自由基的能力,对其光稳定机理也进行了初步的讨论。     

聚集诱导发光基团修饰的功能化树枝形聚合物及其光物理性质研究

构筑和发展新型光功能树枝形聚合物是当前研究热点之一. 聚集诱导发光(Aggregation Induced Emission. AIE)类化合物以其高固态发光量子产率和广阔的应用前景引起研究者的极大关注, 分子内旋转受限降低了非辐射失活被认为是AIE高固态发光量子产率的主要原因. 在树枝形聚合物的外围修饰聚集诱导发光基团, 改善树枝形聚合物的发光性能, 通过外界环境改变树枝形聚合物分子构象, 实现对功能化树枝形聚合物体系发光的调控, 对扩展光功能树枝形聚合物在发光材料以及光捕获体系中的应用有重要意义.     

Computer simulation of polymeric materials. I. Stress-strain behavior

A model of polymeric materials has been developed that includes many of the features of condensed-phase polymer chain dynamics, central among them chain relaxation via conformational motion. The model consists of a number of chains of particles that are connected by bonds with multiwelled potentials to approximate the energetics of conformational motion. Interactions between particles on adjacent chains are modeled by short range repulsive potentials. We have examined the stress-strain behavior of the model using molecular dynamics simulations and find qualitative agreement with the observed experimental behavior of polymeric materials.     

Dynamics and flow-induced phase separation in polymeric fluids

The past few years have seen many advances in our understanding of the dynamics of polymeric fluids. These include improvements on the successful reptation theory; an emerging molecular theory of semiflexible chain dynamics; and an understanding of how to calculate and classify `phase diagrams' for flow-induced transitions. Experimentalists have begun mapping out the phase behavior of wormlike micelles, a `living' polymeric system, in flow: these systems undergo transitions into shear-thinning or shear-thickening phases, whose variety is remarkably rich and poorly understood. Polymeric ideas must be extended to include the delicate charge and composition effects which conspire to stabilize the micelles and are strongly influenced by flow.     

Effects of molecular architectures and solvophobic additives on the aggregative properties of polymeric surfactants

The aggregative behavior of the polymeric surfactants with various molecular architectures in dilute solutions is studied by dissipative particle dynamics. The effects of the solvophobic/solvophilic length, polymeric architecture (linear, star, dendritic, and cyclic type), chain rigidity, and solvophobic additives on the critical micelle concentration (CMC) and the aggregative patterns are systematically investigated. It is found that molecular architectures have a noteworthy impact on the aggregative properties. For linear diblock copolymers, the CMC declines with increasing solvophobic length but rises with increasing solvophilic length. Nonetheless, the solvophobic group has comparatively greater influence on the CMC. Imposition of the star, dendritic, or cyclic structures onto the solvophobic or solvophilic parts of the polymeric surfactant leads to an increase in the CMC. On the contrary, polymers imposed with the greater degree of the rigidity on the solvophobic or solvophilic block have lower CMC. The addition of solvophobic additives results in a decrease of CMC as well. The effects of the concentration and length of the additives on the aggregative behaviors of polymer surfactants were investigated. Interesting supramolecular structures such as caterpillar and worm-like micelles were observed.     

Thermogravimetric studies of polymeric reagents: a polymeric o-benzyne precursor

Thermogravimetry for the study of polymeric reagents is described and used to demonstrate the thermic behavior of a polymeric o-benzyne precursor     

Surface,thermal and mechanical characteristics of polymeric solids

Surface molecular motions of amorphous polymeric solids have been directly measured on the basis of lateral force microscopic (LFM) and scanning viscoelasticity microscopic (SVM) measurements. SVM measurement revealed that the molecular motion at the surface of the monodisperse polystyrene (PS) film with Mn less than ca.30k was fairly activated compared with that in a bulk region, mainly due to the surface segregation of chain end groups. Temperature dependent LFM and SVM measurement revealed that the surface glass transition temperature, Tg of the monodisperse PS film was lower than the bulk one, even though Mn was fairly large as 140k and also, that the time-temperature superposition was applicable to the surface relaxation process. The chain end group segregation at the air/PS interface was verified from the dynamic secondary ion mass spectroscopic (DSIMS) depth profiling of the proton and deuterium ion for the end-labeled deutrated-PS (dPS) film. These results suggest that the surface Tg is depressed due to an increase in free volume near surface region, being induced by the preferential surface localization of chain end groups.     

Rare-earth/inorganic/organic polymeric hybrid materials: molecular assembly, regular microstructure and photoluminescence

2-Hydroxynicotinic acid (HNA) was grafted by 3-(triethoxysilyl)propyl isocyanate (TEPIC) to achieve the molecular precursor HNA-Si through the hydrogen-transfer nucleophilic addition reaction between the hydroxyl group of HNA and the isocyanate group of TEPIC. Then, a chemically bonded rare-earth/inorganic polymeric hybrid material (A) was constructed using HNA-Si as a bridge molecule that can both coordinate to rare-earth ions (HNA-Si-RE) and form an inorganic Si-O network with tetraethoxysilane (TEOS) after cohydrolysis and copolycondensation processes. Further, three types of novel rare-earth/inorganic/organic polymeric hybrids (B-D) were assembled by the introduction of three different organic polymeric chains into the above system. First, methacrylic acid (MAA) [or methacrylic acid and acrylamide (ALM) in the molar ratio of 1:1] was mixed to polymerize (or copolymerize) with benzoyl peroxide (BPO) as the initiator to form poly(methacrylic acid) (PMAA) [or poly(methacrylic and acrylamide) (PMAALM)], and then PMAA or PMAALM was added to the precursor HNA-Si before the assembly of HNA-Si-RE, resulting in the hybrid materials HNA-Si-RE-PMAA (B) and HNA-Si-RE-PMAALM (C). Second, poly(vinylpyrrolidone) (PVP) was added to coordinate to the rare-earth ions by the carbonyl group in the complex HNA-Si-RE, to achieve the hybrid HNA-Si-RE-PVP (D). All of these hybrid materials exhibit homogeneous, regular, and ordered microstructures and morphologies, suggesting the occurrence of self-assembly of the inorganic network and organic chain. Measurements of the photoluminescent properties of these materials show that the ternary rare-earth/inorganic/organic polymeric hybrids present stronger luminescent intensities, longer lifetimes, and higher luminescent quantum efficiencies than the binary rare-earth/inorganic polymeric hybrids, indicating that the introduction of the organic polymer chain is a benefit for the luminescence of the overall hybrid system.     

Monte Carlo simulation of polymeric materials: Recent progress

Monte Carlo simulations are presented, dealing with phase diagrams of block copolymer melts and polymer blends, including the unmixing kinetics of the latter systems. The theoretical background is briefly reviewed: Ginzburg-type criteria reveal that in mixtures of long flexible polymers a “crossover” occurs from mean-field behavior (as described by Flory-Huggins theory) to nonclassical Ising-type behavior, and spinodal curves can be unusually sharp. This crossover is demonstrated by large scale simulations of the bond fluctuation model, and it is also shown that for symmetric mixtures the critical temperature scales with chain length as T_c α N. The prefactor in this relation is distinctly smaller than predicted by Flory-Huggins, but the Curro-Schweizer integral equation theory prediction T_c α √N is clearly ruled out. Tests of the Cahn theory on the initial stages of spinodal decomposition of polymer blends will also be reported. To conclude, the mesophase formation in block copolymers is discussed, and it is shown that the simulations agree very well with experiment. The pronounced chain stretching that already occurs in the disordered phase is compelling evidence against the validity of simple random phase approximation concepts for these systems. This shows how Monte Carlo simulations can assist in better understanding large classes of polymeric materials.     

Foam, emulsion and wetting films stabilized by polyoxyalkylated diethylenetriamine (DETA) polymeric surfactants

This review explores three (A, B, C) polyoxyalkylated diethylenetriamine (DETA) polymeric surfactants belonging to the group of star-like polymers. They have a similar structure, differing only in the number of polymeric branches (4, 6 and 9 in the mentioned order). The differences in these surfactants' ability to stabilize foam, o/w/o and w/o/w emulsion and wetting films are evaluated by a number of methods summarized in Section 2. Results from the studies indicate that differences in polymeric surfactants' molecular structure affect the properties exhibited at air/water, oil/water and water/solid interfaces, such as the value of surface tension, interfacial tension, critical micelle concentration, degree of hydrophobicity of solid surface, etc. Foam, emulsion and wetting films stabilized by such surfactants also show different behavior regarding some specific parameters, such as critical electrolyte concentration, surfactant concentration for obtaining a stable film, film thickness value, etc. These observations give reasons to believe that model studies can support a comprehensive understanding of how the change in polymeric surfactant structure can impact thin liquid films properties. This may enable a targeted design of the macromolecular architecture depending on the polymeric surfactants application purpose.     

The electronic structures of polymeric beryllium hydride and polymeric boron hydride

The band structure of linear polymeric beryllium hydride is here calculated by anab initio technique. The doubly-degenerate valence band has symmetry and is composed of a berylliump orbital and an antisymmetric combination of the appropriate hydrogen 1s orbitals. The Koopmans' ionization potential is calculated to be 16.1 eV and the direct band gap, found atX, is 15.2 eV. The charge distribution shows an electron drift of approximately 0.15 electrons from beryllium to the hydrogen atoms. The total energy calculation indicates that polymeric beryllium hydride is more stable than the monomer while polymeric boron hydride is less stable than the monomeric species. From the polymeric boron hydride system, an alternating-bond model is more stable than a symmetric bond model. The energy band structures of both models reveal that electron delocalization along the polymer chain is weak.     

Influences of chain heterogeneity on instability of polymeric thin films: dewetting of polystyrenes, polychloromethylstyrenes and its copolymers

This study compares the stability of various polymeric thin films supported on SiO(x)/Si substrate. Dewetting behaviors of polystyrenes (PS), polychloromethylstyrenes, and random poly(styrene-co-chloromethylstyrene)s are investigated by utilizing atomic force microscopy. A systematic addition of the chloromethylstyrene (ClMS) unit into PS chain causes the increase of segment polarity, affecting interfacial and interchain interactions in thin films. It is found that stability of the polymeric films depends on two major parameters, ratio of the ClMS unit and film thickness. For approximately 5 nm thick film, the addition of only 5 mol% ClMS unit causes a drastic increase of its stability, attributed to the enhanced interfacial interactions between ClMS group and SiO(x) layer. Further increasing the ClMS mole ratio to 20, 45, and 100% is accompanied by a systematic increase of the film stability. Thicker films (thicknesses approximately 22 and approximately 45 nm) of the copolymer with 5 mol% ClMS unit exhibit rather different behavior. They are found to be less stable compared to the PS films. However, the films of copolymers with ClMS unit of 20, 45, and 100% are still much more stable than the PS films. These dewetting behaviors of the copolymers are correlated to the interfacial interactions, interchain interactions and segmental segregation in thin films.