高聚物玻璃化转变温度和分子参数的关系 Ⅲ·聚甲基丙烯酸甲酯立构规整性和Tg的关系

 本文研究了聚甲基丙烯酸甲酯(PMAA)的立构规整性与T₈的关系,结果表明立构单元分布和含量均对T₈有显著影响。应用前文导出的理论关系,进一步处理了T₈和构象参数实验数据,用这种简单方法计算得的无扰尺寸温度系数和实验值一致。由此推论,不同立构PMMA链的T₈之差反映了它们局部择优链构象的不同。     

冻干保护剂溶液低温退火特性的研究

利用差示扫描量热仪(DSC)研究了10%叔丁醇/10%蔗糖/水溶液的冻结特性, 退火温度及退火时间, 分析了溶液的退火行为. 实验结果表明, 溶液降温时, 蔗糖的存在阻碍了叔丁醇析出, 最大冻结浓缩溶液玻璃化转变温度Tg′由－32.5 ℃降低到－42.0 ℃, 升温时在－30 ℃叔丁醇发生反玻璃化. 在反玻璃化峰附近的温度进行退火可使叔丁醇充分析出, Tg′由－42.0 ℃上升到－34.9 ℃. 所需的退火时间与退火温度有关, 退火温度越接近Tg′, 所需的退火时间越长. 在－37 ℃时, 退火20 min可完全消除反玻璃化.     

高聚物玻璃化转变温度和分子参数的关系 Ⅰ.高聚物链柔性与Tg的关系

 本文采用晶格模型,以动力学链段长度作为统计单元大小,推导了高聚物玻璃化温度T_8和链静态刚性因子σ²(T₈),链动态刚性因子β(T₈)以及聚合度DP等分子参数之间的关系。具体讨论了链柔性对T₈的影响。理论预测和几十种聚合物的实验数据能较好吻合,分析结果表明T₈值基本上取决于高聚物链σ(T₈)大小。     

分子亲脂-亲水性的量子化学描述II. 氨基酸侧链的亲水指标和亲脂指标

在启发式亲脂势HMLP (heuristic molecular lipophilicity potential)的基础上提出了分子、分子片段和原子的亲水指标和亲脂指标. 计算出了20个天然氨基酸侧链的亲水、亲脂指标和亲水、亲脂表面积, 并用线性自由能函数表达氨基酸侧链的溶剂化自由能, ΔG_sol,i^θ＝b₀＋b₁L_i＋b₂H_i＋b₃S_i^＋＋b₄S_i^－. . 应用线性自由能函数和氨基酸侧链的亲水和亲脂指标, 计算了20个氨基酸残基的3种相转移自由能(蒸气-水、蒸气-正辛醇、正辛醇-水)和正辛醇-水分配系数logP_ow, 取得了与实验值高度一致的良好效果. HMLP的亲水和亲脂指标是HMLP的指标化, 扩展了这一方法的使用范围. 氨基酸侧链的亲水、亲脂指标和线性自由能函数有望用于生物大分子受体与配体的结合自由能的估算、蛋白质的结构与功能、蛋白-蛋白相互作用和识别的研究.     

多支型长链均三嗪衍生物的合成与光谱性质

合成了三个较长共轭链的均三嗪类衍生物, 分别为单支的L1、双支的L2、三支的L3, 并与相应的三个较短共轭链的均三嗪类衍生物(S1, S2, S3)做了比较. 实验结果表明, 在弱极性溶剂中, 随着三嗪环上侧链数目的增加或侧链的加长, 吸收光谱和荧光光谱的峰位(λ_max)都发生红移, 吸收强度和荧光强度都显著增强.     

纳米氧化锌的低温热容和热力学性质

用扫描电子显微镜(SEM)测定了纳米氧化锌试样的粒径, SEM结果表明ZnO试样平均粒径为30 nm. 在83～350 K温区, 用精密低温绝热量热计测定了ZnO的等压摩尔热容, 拟合出其等压摩尔热容与热力学温度的函数关系式: C_p＝－3.249＋0.2400T－3.413×10^－4T ²＋4.485×10^－7T ³. 根据热容与热力学函数关系, 计算了以298.15 K为基准的纳米ZnO的热力学函数, 并与粗晶ZnO和18 nm ZnO热容文献报导值进行了比较, 从能量角度分析了不同粒径ZnO热容曲线差别产生的原因.     

导电高分子PEDOT/PSS稳定的Pt3Co纳米粒子的制备及电、磁性

利用一步共还原法在导电高分子聚二氧乙基噻吩/聚对苯乙烯磺酸(PEDOT/PSS)水溶液中合成了磁性纳米复合物Pt₃Co-PEDOT/PSS. 利用透射电镜(TEM)、X射线衍射(XRD)、拉曼光谱、超导量子干涉仪(SQUID)对其进行了表征.结果表明Pt₃Co纳米粒子为面心立方结构(fcc), 粒子平均粒径为9.6 nm, 标准偏差为2.4 nm. 用旋转涂膜法制备的Pt₃Co-PEDOT/PSS薄膜导电率()在1.6～4.0 S/cm之间. 当温度在阻塞温度(T_B, 110.5 K)以上时, 纳米复合物Pt₃Co-PEDOT/PSS显示出超顺磁性, 低于T_B时呈铁磁性, 在5 K时其剩磁(M_r)和矫玩力(H_c)分别为4.1 emu/g和701 Oe(奥斯特).     

联合处理电位法和极谱法得到的实验数据确定金属配合物稳定常数(英)

The cadmium(Ⅱ)-glycinamide system was modeled and its stability constants were calculated by a unified mathematical treatment for experimental data obtained from ion selective electrode (ISE) and differential pulse polarography (DPP). It has been shown that very much the same experimental complex formation curve (ECFC) and theoretical complex formation curve (TCFC) could be given from both experimental techniques for the same experimental conditions, such as the same total ligand c(L_T) and metal ion c(M_T) concentrations. The combination of the two techniques is of many advantages as ISE can be performed at low a c(L_T)∶c(M_T) ratio and significantly higher c(M_T), whereas DPP could be used well at larger the c(L_T)∶c(M_T) ratio and very low c(M_T). This makes it possible to study a metal-ligand system in much broader range of experimental conditions that, in turn, provides us more data and information about the metal-ligand system of interest. Application of the unified mathematical treatment to the cadmium-glycinamide system in this paper, three new complexes MHL, ML₃ and ML₃(OH) as well as two complexes ML and ML₂, reported in literatures, could be modeled and all their stability constants have been refined.     

(GaP)n和(GaP)n－ (n＝10～16)团簇的结构与稳定性研究

采用密度泛函理论B3LYP/Lanl2dz方法对(GaP)_n和(GaP)_n^－ (n＝10～16)团簇的一系列异构体的结构和稳定性进行了研究. 讨论了中性团簇得到一个电子之后, 几何结构和电子性质的变化. 频率分析预测出最强吸收峰位于341～390 cm^－1区域. 从能隙、结合能和能量二次差分等方面综合考虑, 具有T_h对称性的(GaP)₁₂和(GaP)₁₂^－分别是中性(GaP)_n和阴离子(GaP)_n^－团簇中最稳定的, 而具有T_d点群结构的(GaP)₁₆也比较稳定, 究竟哪种结构易于合成还有待于实验的进一步证实. 在相同理论水平上计算了基态(GaP)_n (n＝10～16)的绝热电子亲合势(AEAs)及其基态阴离子的垂直电离能(VDEs), 这对以后的实验数据分析将有一定的参考价值.     

新型一维梯状双链配位聚合物{[Cu(malate)(2,2'-bipy)]•3H2O}∞的合成、晶体结构与表征

合成了铜(II)与羟基丁二酸和2,2'-联吡啶形成的配位聚合物{[Cu(malate)(2,2'-bipy)]•3H₂O}_∞ (其中malate＝羟基丁二酸根, 2,2'-bipy＝2,2'-联吡啶), 通过X射线衍射测定了单晶结构, 并进行了元素分析、红外光谱、紫外光谱、热分析等研究. 配合物属单斜晶系, 空间群P2(1)/c; 晶胞参数: a＝0.70132(10) nm, b＝1.9730(3) nm, c＝1.18998(16) nm, β＝94.551(3)°; Z＝2; 最终偏离因子R＝0.0483. 配合物中每个铜(II)原子与来自2,2'-联吡啶的两个氮原子和两个羟基丁二酸根的三个氧原子配位, 形成畸变的三角双锥结构单元. 每个羟基丁二酸根以R构型方式桥联两个三角双锥结构单元, 沿a轴方向无限延伸形成一维链. 两条平行链以面对面的方式重叠, 彼此吡啶环之间存在强的(-(相互作用, 加之C_吡啶环—H…O_羧基弱相互作用形成新颖的梯状双链结构, 比邻的梯状双链又通过分子间O_羟基-H…O_羧基氢键沿a轴方向共同构筑了具有隧道的三维结构.     

聚丙烯酸酯的玻璃化温度的定量结构性质相关研究

提出了高分子的侧基顺拉模型 ,认为侧基的空间效应主要来源于侧基的轴向横截面积 .与侧基的轴向横截面积密切相关的是侧基的碳链分支数 .直接采用侧基碳链分支数作为侧基的空间效应参数 ,对 13种聚丙烯酸酯和 9种聚甲基丙烯酸酯的玻璃化温度进行了定量结构 性质相关研究 ,得到了良好的三参数模型 ,对聚丙烯酸酯和聚甲基丙烯酸酯的玻璃化温度分别进行回归分析 ,相关系数R2 =0 989(s =3 8K)和R2 =0 993 (s =4 8K) .该模型对 2 2种聚丙烯酸酯和聚甲基丙烯酸酯的合并计算的结果是R2 =0 980 (s =8 3K) .建立的模型参数计算简便 ,模型的稳定性和适应性较好 ,所有模型的标准误差均小于或接近实验误差 .     

New side chain liquid crystalline polymers: synthesis and thermal properties of side chain polyacrylates having segmented spacers

In order to acquire high mobility of a mesogenic group, we propose a new type of side chain liquid crystal polymer having segmented spacers, consisting of binary moieties of an oligo(ethylene oxide) segment and analkylene segment. Six kinds of polyacrylates having segmented spacers consisting of different lengths of an oligo(ethylene oxide) and an alkylene, and having 4'-cyanobiphenyl as a mesogenic group have been synthesized, and their thermal properties investigated. Some of these polyacrylates exhibit a mesophase and show an extremely low glass transition temperature compared with LC polyacrylates having ordinary alkylene spacers.     

New side chain liquid crystalline polymers: synthesis and thermal properties of side chain polyacrylates having segmented spacers

In order to acquire high mobility of a mesogenic group, we propose a new type of side chain liquid crystal polymer having segmented spacers, consisting of binary moieties of an oligo(ethylene oxide) segment and analkylene segment. Six kinds of polyacrylates having segmented spacers consisting of different lengths of an oligo(ethylene oxide) and an alkylene, and having 4'-cyanobiphenyl as a mesogenic group have been synthesized, and their thermal properties investigated. Some of these polyacrylates exhibit a mesophase and show an extremely low glass transition temperature compared with LC polyacrylates having ordinary alkylene spacers.     

交联对聚己二酸乙二醇酯聚氨酯/甲基丙烯酸甲酯交联聚合物的力学阻尼、相容性及形态的影响

用紫外光聚合方法制备出一系列端乙烯基聚己二酸乙二醇酯聚氨酯(PEAPU)和甲基丙烯酸甲酯(MMA)AB交联聚合物(ABCP)。用粘弹谱仪、透射电子显微镜(TEM)和平衡溶胀法研究了AB交联聚合物的动态力学性能、玻璃化转变温度、形态和交联密度、观察到相应于聚氨酯和PMMA相两个玻璃化转变温度,TEM照片中的微相分离是更明显的,ABCP中的两个T_g内移表明,两种成分的化学交联增加了相互的可混性、与ABCP具有相同组成的IPN有比ABCP大得多的相区。氢键能够影响ABCP的相容性、形态和动态力学性能。     

交联对聚己二酸乙二醇酯聚氨酯/甲基丙烯酸甲酯交联聚合物的力学阻尼、相容性及形态的影响

 用紫外光聚合方法制备出一系列端乙烯基聚己二酸乙二醇酯聚氨酯(PEAPU)和甲基丙烯酸甲酯(MMA)AB交联聚合物(ABCP)。用粘弹谱仪、透射电子显微镜(TEM)和平衡溶胀法研究了AB交联聚合物的动态力学性能、玻璃化转变温度、形态和交联密度、观察到相应于聚氨酯和PMMA相两个玻璃化转变温度,TEM照片中的微相分离是更明显的,ABCP中的两个T_g内移表明,两种成分的化学交联增加了相互的可混性、与ABCP具有相同组成的IPN有比ABCP大得多的相区。氢键能够影响ABCP的相容性、形态和动态力学性能。     

Unusual electro-optical behaviour of the nematic polyacrylate

ABSTRACT

High sensitivity of liquid crystals to the electric field makes them highly demanded and widely used in different applications. Despite the large number of the electro-optical research on the low-molar-mass liquid crystals electro-optics of the liquid crystalline (LC) polymers is much less studied. Herein, the comparative electro-optical behaviour of two nematic comb-shaped polyacrylates with phenylbenzoate mesogenic side groups was studied in detail. These two polyacrylates have completely the same structure of polymer backbone and spacer length but different in the direction of the ester group in the phenylbenzoate fragments. It was found that this difference predetermines their completely opposite electro-optical properties.

The influence of the electric field of different strength and frequency on the orientation of the mesogenic groups of these polymers is studied. It is shown that application of the electric field at temperatures above the glass transition temperature (~25°C) induces reorientation of the mesogenic groups along or perpendicular to the electric field direction depending in its turn on the ester group direction. For one of the polyacrylates an unusual textural transition is found; during cooling of the polymer sample under applied field at definite temperature a sharp change in the mesogen’s orientation from homeotropic to planar one is found. This electro-optical phenomenon is observed for the first time and probably associated with sharp change in sign of anisotropy of dielectric permittivity from positive (at high temperatures) to negative one (at lower temperatures). Kinetics of the electro-optical switching at different temperatures, influence of the molar masses of the polymer and frequency of the applied AC field on electro-optical behaviour of the polymers are studied. The possibility of the fixation of the electroinduced homeotropic alignment of the mesogenic groups by photopolymerisation of the diacrylate dissolved in the polymer is demonstrated.