5-{[(4′-正戊基氧-4-联苯基基)羰基]氧}-1-戊炔的相转变与相结构

采用差示扫描量热(DSC)、一维(1D)广角X射线衍射(WAXD)、热台偏光显微镜(PLM-hotstage)等研究手段对含联苯液晶基元的侧链液晶聚炔单体5-{[(4′-正戊基氧-4-联苯基基)羰基]氧}-1-戊炔(A3EO5)的本体相转变和相结构进行了研究.DSC和1D-WAXD实验结果表明,A3EO5在升温和降温过程中均呈现四个相转变过程,形成双向性液晶.样品从各向同性态降温至室温过程中,首先形成近晶A相,随后进入层内排列具有准长程有序的近晶B相,继续降温将形成层内为正交排列的近晶E相,在此之后样品进入晶相.PLM结果指出样品在各向同性态降温过程中分别形成球状织构、角锥织构和同心圆弧织构.     

聚｛11-[(4′-正庚氧基-4-联苯基)羰基]氧-1-十一炔｝的相结构与相转变

采用示差扫描量热法(DSC)、一维(1D)、二维(2D)广角X-射线衍射(WAXD)和偏光显微镜(PLM)等研究手段对聚{11-[(4′-正庚氧基-4-联苯基)羰基]氧-1-十一炔}(PA-9,7)的本体相转变和相结构进行研究,并采用分子动力学方法对相结构进行模拟.结果表明,样品的相转变为近晶B相(SmB)近晶A相(SmA)各向同性态(Iso).在近晶B相中,侧链在层状结构中排列成具有六次对称性的准长程有序结构。     

聚{11-[(4'-正庚氧基-4-联苯基)羰基]氧-1-十一炔}的相结构与相转变

采用示差扫描量热法(DSC)、一维(1D)、二维(2D)广角X-射线衍射(WAXD)和偏光显微镜(PLM)等研究手段对聚{11-[(4'-正庚氧基-4-联苯基)羰基]氧-1-十一炔}(PA-9,7)的本体相转变和相结构进行研究,并采用分子动力学方法对相结构进行模拟.结果表明,样品的相转变为近晶B相(SmB)(→)近晶A相(SmA)(→)各向同性态(Iso).在近晶B相中,侧链在层状结构中排列成具有六次对称性的准长程有序结构.     

不同分子量聚丙烯β晶相的形成

结晶速率;晶相转变;不同分子量聚丙烯β晶相的形成     

结晶聚合物晶相相容性的研究

通过ＤＳＣ、Ｘ－射线衍射、红外光谱及拉伸试验研究了ＨＤＰＥ与ＬＬＤＰＥ、ＨＤＰＥ与ＬＤＰＥ之间的晶相相容性。结果表明，链结构相近的ＨＤＰＥ和ＬＬＤＰＥ的晶相相容性好，能形成共晶，而链结构差异较大的ＨＤＰＥ和ＬＤＰＥ的晶相相容性较差，倾向于分别结晶。但有部分链段被对方的晶区夹持。不论是支化度大的ＬＤＰＥ锻段插入以ＨＤＰＥ为主的晶区，还是支化度小的ＨＤＰＥ锻段插入以ＬＤＰＥ为主的晶区，都可破坏晶区的规     

偏氟乙烯-四氟乙烯共聚物的β、γ混合晶型固相转变与松弛现象

本文用红外光谱及压电常数方法研究了偏氟乙烯-四氟乙烯共聚物在高压直流电场下,γ晶型向β晶型的固相转变。同时用动态力学方法、介电损耗测试法及压电常数方法研究了样品的松弛现象。     

YBa2Cu3O7—x超导化合物在加热过程中相转变的高压电镜原位观察

对YBa_2Cu_3O_(7-x)超导化合物在加热过程中的相转变进行了高压电镜原位观察,并做了在空气中的X射线衍射分析和真空处理样品的X射线衍射物相分析。结果表明,在真空环境下,相变温度与氧含量有关,一般比在空气中低100～120℃。在320～350℃,孪晶带开始消失,在样品表面出现一些Cu_2O黑斑,并开始由正交结构YBa_2Cu_3O_(7-x)向正交结构Y_2BaCuO_5化合物转变,在500℃左右相转变结束。在冷却过程中未发现相转变。     

单斜与锐钛矿双晶相TiO2的水热法制备与机理探讨

以一种具有超强耐酸碱的表面活性剂-丁基封端脂肪醇聚氧乙烯醚作为晶型调节剂,利用钛酸丁酯和氢氧化钠的水热反应制备了双晶相(单斜相与锐钛矿相)TiO2,考察了丁基封端脂肪醇聚氧乙烯醚和钛酸丁酯的物质的量比R、反应时间、反应温度等因素对产物的晶相组成的影响,并对不同条件下的晶相转变机理进行了初步探讨。     

晶相调控对金属纳米粒子催化性能的影响

尺寸在1–10 nm的金属纳米催化剂广泛地应用于石油化工,精细化学品合成,能源与环境保护等领域。大量研究表明,金属纳米粒子的催化性能与其微观结构,即尺寸、形貌和晶相等密切相关。近年来,对金属纳米粒子的尺寸和形貌效应已经有了较为系统深入的研究,但对晶相效应的研究则较少涉及。这主要是由于介稳晶相的金属纳米粒子在合成过程中或反应条件下极易转化为热力学稳定的晶相结构。根据金属原子密堆积形式,金属纳米粒子的晶相结构主要有立方面心(fcc)、立方体心(bcc)和六方密堆积(hcp)三种晶相;而金属合金由于d带电子存在着多种杂化方式,因而其晶相结构呈现出多样性且与单一金属有很大的不同。金属和合金纳米粒子晶相结构的调控,不仅会改变金属原子的配位环境,调控了其电子分布状态,还可影响反应物和产物的吸附、活化和脱附,进而调变催化性能。首先,我们简要总结了液相合成和固相转变调控金属纳米粒子晶相的原理和方法。纳米粒子的液相合成一般包括前驱体还原成核和晶核生长两个阶段,通过对液相合成条件的优化,尤其是表面活性剂的选择,可有效调控合成过程中的热力学和动力学因素,从而实现金属晶相的可控合成。固相转变则主要是对具有一定晶相结构的纳米粒子于一定气氛和温度条件下进行加热处理,利用金属粒子与活性气体之间(H2, CO等)的化学作用来实现晶相转变。利用上述方法,可以合成出fcc-Co、fcc-Ru、L10-AuCu等热力学介稳的金属或合金纳米粒子。在此基础之上,我们分别以Co纳米粒子(fcc和hcp晶相)催化FT合成, Fe模型催化剂(fcc和bcc晶相)活化N2和CO, Ru纳米粒子(fcc和hcp晶相)催化CO氧化和氨硼烷水解制氢, Pd纳米粒子(PdHx物种)催化加氢等为例分析了晶相对金属纳米粒子催化性能的影响;在合金催化剂方面,以Pt3Co(无序的fcc和有序的L12), AuPdCo(P3–m、Fm3–m和R3–m混合晶相)和FePt纳米粒子(fcc和fct相)催化O2电化学还原、PtRhSn (碲铂矿晶相和fcc晶相)和ZrPt3纳米粒子(hcp和fcc晶相)催化乙醇电氧化、Ag3In合金(无序的Fm3–m相和有序的Pm3–m晶相)催化对硝基苯酚加氢、PdRu纳米粒子(fcc和hcp混合晶相)催化CO氧化等为例分析了合金催化剂的晶相对催化性能的影响。上述研究进展表明,金属纳米粒子的晶相也是影响制备剂高效金属催化剂的主要因素。最后,我们结合纳米催化的发展现状,提出了金属纳米粒子的晶相调控在纳米催化和纳米材料领域可能的发展态势。第一,通过对金属纳米粒子溶液相合成机理的深入研究,有助于发展出尺寸、形貌和晶相同时可控的新合成方法。第二,金属纳米粒子在晶相转化过程中往往伴随着烧结及组分的偏析等难题。利用氧化物包覆的核壳型或蛋壳型纳米结构以及碳纳米管的空间限域效应,或许有助于解决上述难题。第三,具有亚稳晶相结构的金属纳米粒子在反应条件下极易转变为热力学稳定的结构,因此,利用原位、动态、实时的表征技术对催化剂在真实工作状态下的微观结构进行细致的分析是阐明晶相效应的前提。     

固相剪切碾磨方法制备聚丙烯/钛酸钡高介电常数复合材料

采用固相剪切碾磨方法(S3M)制备高介电常数聚丙烯/钛酸钡复合材料。当钛酸钡体积分数φBaTiO3=0.50时,体系的介电常数由纯聚丙烯的2.3增加到108.7(1 kHz)。复合材料断面的SEM照片显示,粒径约100 nm的钛酸钡粒子均匀分散在聚丙烯基体中。复合粉体的SEM、TGA和FT-IR分析表明固相剪切碾磨产生的强大剪切、挤压、摩擦等作用在聚合物相引起多种复杂的物理及化学变化,聚合物粒径变小,粒子比表面积增大,表面能大幅增加,与具有较高表面活性的钛酸钡粒子形成较强的界面相互作用。     

葡萄糖苷特异性固相萃取固定相的合成、表征及应用

以马来酰亚胺基修饰凝胶载体,通过β-葡萄糖胺和2-亚氨基硫代烷盐酸盐将作为配基的β-葡萄糖脒连接到载体上,合成了一种葡萄糖苷特异性固相萃取固定相,并对其固相萃取性能进行了表征.该固定相对葡萄糖苷具有特异性识别,并成功用于固相萃取分离葡萄糖苷.     

反相液相色谱中固定相和流动相对柱相比的贡献

依据柱相比的热力学定义和反相液相色谱中溶质的计量置换保留理论(the stoichiometric dispheement heory of solute for retention，SDT-R)，对反相液相色谱中固定相和流动相性质、温度对柱相比的影响进行了研究。结果表明：固定相的种类和配基的疏水性对柱相比影响较大，而流动相中有机溶剂的种类，特别是脂肪酸作为置换剂时，对柱相比的影响更大，而柱相比受温度的影响较小。此外，通过用27种小分子溶质对柱相比的测定，其logI和Z良好的线性关系，进一步证明柱相比是一个与溶质性质无关的常数。     

Morphological studies of a hydrogen-bonded LC polymer obtained by photopolymerization in LC solvents

Anisotropic morphologies and the phase behaviour of a hydrogen-bonded LC polymer obtained by photopolymerization in two kinds of LC solvent are discussed. The hydrogen-bonded LC monomer, 4-(6-acryloyloxyhexyloxy) benzoic acid (A6OBA), was photopolymerized in 4-cyano-4′-hexyloxybiphenyl (6OCB) and in 4-cyano-4′-undecyloxybiphenyl (11OCB), which show a nematic phase and a smectic A phase, respectively. After photo-polymerization, the LC media were removed by extraction and the pure polymer was observed by scanning electron microscopy. SEM images showed that the polymer possessed fibrous morphology with a fibre diameter of a few micrometers, based on polymerization-induced phase separation. The overall geometries reflected typical LC characteristics such as schlieren and focal-conic fan textures. It was found that the hydrogen bond between benzoic acid groups in the monomer was rigid enough to fix the anisotropic phase-separated structure forming during the early stage of phase separation; however, it could not permanently maintain the fibre structure due to dissociation at elevated temperature. X-ray measurements revealed that a well developed layer structure of the hydrogen-bonded mesogen existed in the polymer obtained from the smectic phase of 11OCB, whereas a polymer layer structure could develop only partially from the nematic phase of 6OCB.     

Cholesterol-based dimeric liquid crystals: synthesis,mesomorphic behaviour of frustrated phases and DFT study

Chiral unsymmetrical dimeric liquid crystals consisting of a cholesterol moiety as chiral entity and a substituted salicylidene imine core (with the substituent being butyl or fluoro or chloro group) interconnected through an even methylene spacer have been synthesised and their mesomorphic properties are characterised. All the dimers exhibit enantiotropic mesophases. The butyl homologue exhibited N* phase only, the fluoro- and chloro-substituted compound exhibited frustrated blue phases (BPs), N* phase and SmC* or twisted grain boundary (TGB) phases. The occurrence of a fluid frustrated phase, the BP, in particular, observed in compounds with a polar moiety and bent optimised conformation by density functional theory (DFT) study, indicates the importance of polar structures and bent shape of the compounds. Theoretical calculation was performed in order to study the optimised conformation, polarity and electron density distribution of the synthesised cholesterol derivatives using DFT. Time-dependent density functional theory (TD-DFT) calculation also had been carried out to investigate the absorption spectra and HOMO–LUMO energies. The experimental and theoretical absorption spectra are also presented.     

Preorganised effects of a tetramesogenic supermolecule on supramolecular assembly in the liquid crystalline phases

After preparing a homologous series of tetrameric mesogenic compounds in which two U-shaped molecules were connected via a rigid benzene derivative or a flexible alkyl chain, we investigated their phase transition behaviour using optical microscopy, differential scanning calorimetry and X-ray diffraction analysis. The compounds possessing an alkyl spacer as the central group exhibited nematic and smectic A phases just as the corresponding U-shaped molecule did. The compound possessing a 1,2-benzene unit as the connecting group showed nematic and smectic A phases, although the compound possessing a 1,3-benzene unit exhibited only an anticlinic smectic C phase. Structure–property relations of the liquid crystalline tetramers are interpreted in terms of preorganised effects of the four mesogenic units.     

亲水有机相-含盐水两相体系的形成机理与分相能力

亲水有机相-含盐水两相体系的形成机理与分相能力;亲水有机相;含盐水相;两相体系;分相机理;分相能力     

Oxadiazole-based unsymmetrical chiral liquid crystal dimers: synthesis and mesomorphic properties

The synthesis and liquid crystalline properties of novel chiral Schiff's base dimers containing the 1,3,4-oxadiazole ring are reported. The length of the terminal S-alkyl chain has been varied. All the compounds synthesised were thermally stable and exhibited enantiotropic mesomorphism, showing either SmC*–SmA–TGB–N*–BP or SmC*–SmA phase sequence.     

Time‐Resolved Phase Transitions of the Nanocrystalline Cubic to Submicron Monoclinic Phase in Zirconia

The nanocrystalline cubic, tetragonal, and submicron monoclinic phases of pure zirconia were prepared by thermal decomposition of carbonate and hydroxide precursors. The crystallization and isothermal phase transformations of the oxide were studied using high temperature X‐ray diffraction, X‐ray diffraction and Raman spectra of quenched samples. Cubic zirconia formed first, and then progressively transformed to tetragonal and monoclinic phases at temperatures as low as 320°C. The cubic, tetragonal, and monoclinic phases for ZrO₂ were found to be distinct functions of crystallite size, indicating the nanocrystalline nature of these phases. They were found to exist within critical size ranges of 50 to 140 Å, 100 to 220 Å and 190 to 420 Å (±5 Å), respectively. Thus, as the crystallites grow during annealing, they first transform from cubic to tetragonal and then from tetragonal to monoclinic at critical sizes. The classical Avrami equation for nucleation and growth was applied to the tetragonal to monoclinic phase transition.     

Physical properties of two systems with induced antiferroelectric phase

Two ferroelectric three‐ring chiral esters, one with a partially fluorinated alkyl chain and another with a cyano terminal group, were mixed with a structurally similar compound having an alkyl terminal chain. In their mixtures an antiferroelectric phase was induced. The phase behaviour, spontaneous polarisation, tilt angle, smectic layer spacing and helical pitch of both systems were determined. The mechanism of the induction of an antiferroelectric phase is different in both cases, with highly tilted phases in former system and less tilted phases in the latter.     

Phase equilibria in the GeSe2-SnTe system

Journal of Thermal Analysis and Calorimetry - The phase diagram of the system GeSe2-SnTe is studied by means of X-ray diffraction, differential thermal and measurements of the microhardness and the...