木质素基偶氮聚合物胶体球的制备

利用造纸废液中的碱木素(AL)合成了木质素基偶氮聚合物(AL-azo-COOEt), 并研究其自组装胶体化过程. 木质素偶氮聚合物的成功合成通过核磁共振氢谱(¹H NMR)、紫外-可见(UV-Vis)光谱、傅里叶变换红外(FTIR)光谱和元素分析等表征方法得到证实. 激光光散射(LLS)监测了AL-azo-COOEt的胶体化过程, 自组装形成的胶体球利用透射电镜(TEM)、扫描电镜(SEM)、X射线光电子能谱仪(XPS)和元素分析等进行表征. 结果表明,木质素偶氮聚合物通过疏水聚集作用可以形成规整的实心胶体球, 且为内部较疏水外部较亲水性质的结构. 木质素偶氮聚合物胶体球可以包载疏水性药物阿霉素(DOX), 且其缓释性能可以通过缓冲溶液的pH值来调控.     

双组分偶氮聚合物胶体球制备及其光致形变行为研究

研究了2种环氧树脂类含4-氨基-4′-硝基偶氮苯和4-氨基-4′-羧基偶氮苯生色团聚合物（BP-AZ-NT、BP-AZ-CA）双组分胶体球的制备和光致形变行为.通过在上述聚合物的四氢呋喃溶液中逐步加水诱导自组装的方法,得到了BP-AZ-CA/BP-AZ-NT双组分胶体球.在上述两种聚合物自组装形成胶体球过程中,较为疏水的BP-AZ-NT分子先发生聚集,而较亲水的BP-AZ-CA则在形成的胶体颗粒表面发生进一步聚集.在胶体球形成过程中,体系的临界水含量（CWC）主要由BP-AZ-NT发生聚集时的水含量决定,双组分胶体球的外层则含较多的BP AZ-CA分子.比较单组分胶体球与双组分胶体球在线偏振Ar+激光（488 nm,100 mW/cm2）照射下的形变行为,进一步证实了通过上述方法可以制备BP-AZ-CA和BP-AZ-NT双组份的胶体球;胶体球形变时的初始拉伸速率由胶体球的外层聚合物分子的性质所决定.     

偶氮苯基两亲性聚合物的自组装行为研究进展

偶氮苯基两亲性聚合物结合了偶氮苯基团的光响应、酶响应、主客体识别特性和两亲性聚合物的自组装特性,能够在选择性溶剂中发生聚合物可控自组装行为,这使得其在药物控释、纳米技术和生物医学材料等领域受到了广泛的关注。本文从结构类型和合成方法出发,综述了新型偶氮苯基两亲性聚合物在溶液中的自组装研究进展,并对该领域的发展前景进行了展望。     

偶氮苯超支化聚合物的自组装及其光响应性

采用“A2+B2B'”单体的迈克尔加成聚合方法制备了一类新型的偶氮苯超支化聚合物(HPAzoAMAM).借助扫描电镜(SEM)、透射电镜(TEM)、动态光散射(DLS)和紫外-可见吸收光谱(UV-Vis)等研究了HPAzoAMAM在水溶液中的自组装形貌和光响应性.结果 表明:所得HPAzoAMAM能够组装成大复合胶束,...     

含偶氮苯侧链分子刷聚合物的合成及其光响应自组装

分子刷聚合物伸展的高分子主链、高密度的侧链和较低的侧链空间缠结,使其展现出独特的流变学、力学性能和特殊的分子聚集状态,在纳米技术、表面科学等领域有着广泛的应用前景.基于同时含有2-羰基溴与炔基基团的大分子试剂聚2-((2-溴代丙酰氧基)甲基)丙烯酸丙炔酯,引发偶氮苯丙烯酸酯单体的原子转移自由基聚合(ATRP)与叠氮功能...     

含偶氮苯生色团的聚合物纳米微球的制备与表征

用质子化的4-乙烯基吡啶-丙烯腈无规共聚物(P4VP+-r-AN)与偶氮苯染料酸性间胺黄(MY)在水溶液中通过静电力作用制备了一种新型的侧链偶氮复合物(P4VP-r-AN/MY). 采用FTIR, UV-Vis, DSC, TEM和HRTEM-EDS研究了溶剂对P4VP-r-AN/MY聚集形态的影响, 并初步探讨了P4VP-r-AN/MY聚集体的形成过程及转变机理. 结果表明, P4VP-r-AN/MY在水溶液中聚集形成尺寸为10~250 nm的球形聚集体; 在DMF中, 球形聚集体解聚, 形成较为均匀的薄膜结构; 而向P4VP-r-AN/MY的N,N′-二甲基甲酰胺(DMF)中逐渐增加水的含量, P4VP-r-AN/MY又会重新聚集, 当含水量达到质量分数为62.5%时, P4VP-r-AN/MY聚集形成尺寸为30~200 nm的空心纳米球. 溶剂的组成(水和DMF的质量比)对P4VP-r-AN/MY聚集体形态起着至关重要的作用.     

偶氮液晶嵌段共聚物自组装和光响应性研究进展

偶氮液晶嵌段共聚物是指分子中带有偶氮苯基团的液晶嵌段共聚物.偶氮液晶嵌段共聚物兼具偶氮聚合物的光响应性和液晶嵌段共聚物自组装形成多尺度有序结构的特性,是一类有重要应用前景的新材料.本文简要综述了近10年来偶氮液晶嵌段共聚物的研究进展,以几种典型的偶氮液晶嵌段共聚物为例,介绍嵌段共聚物在本体以及溶液状态下自组装,自组装形貌的光致变化,以及偶氮液晶嵌段共聚物在光全息存储领域等的研究进展.     

无皂乳液聚合制备光敏聚合物微球及其光响应性

利用红外光谱(IR)和核磁共振(1H NMR)对所制备的光敏可聚合单体重氮萘醌苯磺酸甲基丙烯酸羟乙酯(DNQMA)进行了表征. 采用无皂乳液聚合方法制备DNQMA与甲基丙烯酸叔丁酯(t-BMA)的共聚合光敏微球. 利用紫外光谱(UV/Vis)、动态光散射(DLS)、扫描电镜(SEM)对光敏微球在光照前后形态的变化进行了表征. DLS的研究结果表明在水分散液中, 光敏微球的尺寸随光照时间的增加, 先增大, 然后达到平衡. 这与紫外光谱中DNQMA特征吸收达到饱和的时间相一致. SEM研究结果表明光敏微球的形态在光照后破坏很严重, 并基本解体.     

离子自组装方法在偶氮光响应材料制备中的应用

偶氮光响应材料在光信息存储,光学器件制造等领域具有广阔的应用前景。离子自组装技术是近几年发展起来的制备超分子功能材料的一种新方法。本文首先对偶氮光响应材料的制备方法以及离子自组装技术的基本原理做了简单的介绍。然后分4类对离子自组装方法在偶氮光响应材料制备中的应用进行了综述,主要包括带电荷小分子染料与反电荷表面活性剂组装、聚电解质与反电荷偶氮小分子组装、高支化大分子与偶氮小分子组装以及环糊精与含偶氮聚电解质组装。最后对该领域的发展趋势和研究热点进行了展望。     

光响应性偶氮聚电解质自组装研究

将3种侧链带有不同偶氮生色团的聚电解质,用逐层浸渍的方法使其组装成多层膜.利用原子力显微镜(AFM)研究了自组装膜的表面形貌以及随着组装层数增加的变化.详细研究了在紫外光的照射下,薄膜内偶氮生色团由反式到顺式构型的光响应转变,以及在暗室中由顺式回复到反式构型的回复特性.与自组装膜的光响应性和相应的旋涂膜进行比较发现,其中的PNAPE/PDAC自组装膜没有明显的光色效应,而PEAPE/PDAC,PPAPE/PDAC具有明显的光色效应.在暗室中,随生色团的结构不同和在不同的凝集态中,由顺式回复到反式构型的速率明显不同.     

Structural and dynamic properties of colloidal liquids and gases of silica spheres (29 nm in diameter) as studied by the light scattering measurements

Static and dynamic light-scattering measurements are made for colloidal-liquids and -gases of silica spheres (29 nm in diameter) in the exhaustively deionized aqueous suspension and in the presence of sodium chloride. Single broad peak is observed in the light-scattering curve and the liquid-like and gas-like distributions have been observed. Colloidal crystals are not formed at any sphere concentrations. The nearest-neighbored interparticle distances of colloidal liquids, l _obs , agree excellently with the effective diameters of spheres (d _eff ) including the electrical double layers in the effective soft-sphere model and also with the mean intersphere distances, l _o , calculated from the sphere concentration, i.e., l _obs ≈d _eff ≈ l _o . This relation supports the importance of the electrostatic interparticle repulsive interaction. Two dynamic processes have been extracted separately from the time profiles of autocorrelation function of colloidal liquids. Decay curves of colloidal gases are characterized by the single translational diffusion coefficients, which are always lower than the calculation from the Stokes-Einstein equation using true diameter of spheres and increase as ionic concentration increases. These experimental results emphasize the importance of the expanded electrical double layers and the electrostatic intersphere repulsion on the structural and dynamic properties of the colloidal liquids and gases. Electronic Publication     

Simultaneous determination of particle size and density in polydisperse colloidal samples by sedimentation field-flow fractionation

Sedimentation Field-Flow Fractionation (SFFF), which is a one-phase chromatographic system, is shown to be a rapid and convenient method for the simultaneous determination of particle size and density in polydisperse colloidal samples. This can be done by a methodology based on the variation of the carrier solution density using various aqueous glycerol solutions having different concentrations. A polydisperse polyvinyl chloride (PVC) latex sample was used as a model colloid. The average diameters and densities found by the proposed methodology are in good agreement with those obtained from the normal. SFFF procedure using a carrier of constant density or given by the manufacturer. Number average, d_N, and weight average, d_w, particle diameters were determined for the PVC sample at various carrier solutions containing glycerol up to 40 % (w/w) in order to show whether sample aggregation has occurred or not in the presence of glycerol. In all cases, the ratio d_w/d_N was found to be constant, showing that PVC aggregation has not occurred. Therefore our results, obtained by the proposed methodology in SFFF, are accurate, showing that this approach has considerable promise for characterizing complex colloidal materials.     

Rigidity of colloidal crystals of silica spheres modified with polymers on their surfaces in organic solvents

Rigidity (G) of colloidal crystals in organic solvents of acetonitrile and nitrobenzene has been measured by reflection spectroscopy in sedimentation equilibrium. The colloidal spheres used are the silica spheres (136 nm in diameter) modified on their surfaces with polymers, poly(maleic anhydride-co-styrene) [P(MA-ST)], poly(methyl methacrylate) (PMMA), or polystyrene (PST). Log G increases linearly with the slope of unity as log N (number density of colloidal spheres) increases. The mean values of the b-factor, which is the fluctuation parameter in crystal lattices and should be smaller than 0.1 according to the Lindeman's rule, are 0.045±0.003, 0.039±0.007, and 0.038±0.003 for P(MA-ST)/SiO₂, PMMA/SiO₂, and PST/SiO₂, respectively. These values are larger than that of colloidal crystals of mother silica spheres in the deionized aqueous suspension, 0.028. These results support the important role of the excluded volume effects from the polymer layers formed around the silica surfaces. However, contribution of the excluded volume effects from the electrical double layers formed around the spheres in the organic solvents is also effective in the colloidal crystallization. Electronic Publication     

新型氧化铝空心球的制备及表征

以胶体碳球为模板, 廉价的硝酸铝为铝源, 成功制备出了新型的大小可控的氧化铝空心球. 通过透射电子显微镜(TEM)、扫描电子显微镜(SEM)、能量扩散X射线(EDX)、X射线粉末衍射(XRD)等手段对合成产品进行了表征, 并考察了不同合成条件对空心球形貌的影响. 实验结果表明, 合成的氧化铝空心球大小均一, 粒径及壁厚均可调节. 在该实验条件下, 硝酸铝浓度及吸附时间的改变对产品结果没有明显的影响, 而吸附温度的改变引起了产品表面光滑度及壁厚的改变.     

Video-tape observation of the crystal growth and morphology of colloidal single crystals

Crystal growth and morphology of colloidal crystals of silica spheres (81.2 nm in diameter) are observed directly on a video-tape camera. Crystal growth from the round-shaped, small single crystals to the angular-shaped ones is clear. It is observable that the single crystals are packed densely and separated from each other with the grain boundaries. The morphology of colloidal crystals is quite similar to that of typical crystals such as metals, proteins, and ice.     

侧链偶氮聚电解质在胶体微球表面的静电层层自组装和微胶囊制作

将侧链偶氮聚电解质应用于聚苯乙烯胶体微球表面的静电层层自组装, 得到了偶氮聚电解质和聚二烯丙基二甲基氯化铵多层膜覆盖的核壳微球.实验表明, 组装后偶氮苯基团发生了一定程度的解聚集, 得到的胶体微球可表现出明显的光色效应.研究进一步采用含肉桂酸酯的光敏聚电解质作为交联的保护壳层, 并通过光交联反应使表面层发生交联固化反应.将上述具有核壳结构的胶体球溶解去除聚苯乙烯内核后, 得到了含光响应聚电解质的空心微胶囊.     

Another look at the melting temperature of colloidal crystals in the completely deionized suspension

Melting temperature (T _m) of colloidal crystals of monodispersed polystyrene and silica spheres has been measured for thecompletely deionized suspensions as a function of sphere concentration. More than 3 weeks are needed before achievement of the completely deionized state.T _mincreases substantially as the deionization process of the suspension proceeds. The most reliable values ofT _mobserved for the completely deionized suspensions are successfully analyzed again with the theory of Williams et al. The newT _mvalues are compared also with the theory of Robbins et al., which treats the repulsive Yukawa potential between colloidal spheres.     

Large single crystals of colloidal silica spheres appearing in deionized and diluted suspension

Close-up color photographs are taken for crystallites (single crystals surrounded by the grain boundaries) in the colloidal crystals of monodisperse silica spheres (diameter: 110 nm±4.5 nm (standard deviation)). Very large crystallites (34 mm) are observed with the naked eye (for the first time) for the completely deionized and diluted suspensions. Deionization is carefully made with the mixed beds of ion-exchange resins more than 2 weeks old. Size of the crystallites increases sharply as the concentration of spheres decreases, and becomes small at the concentrations slightly higher than the critical concentration of melting toward liquid-like structure. Shape of the crystallites, i.e., mixture of triangle, cubic, pentagonal, hexagonal, cone-like, etc., is recognized in the photographs.     

微凝胶胶体晶体研究进展

Poly(N-isopropylacrylamide)(PNIPAM)微凝胶粒子是一种软的胶体粒子.和单分散的SiO_2、PS、PMMA等硬的胶体粒子一样,单分散的PNIPAM微凝胶粒子也可以自组装成为高度有序的胶体晶体.微凝胶粒子软物质的特性及其对外部刺激的响应性赋予其不同于硬球的组装行为.微凝胶胶体晶体的高度有序结构及其刺激响应性使其在诸多领域有重要用途.本文分别介绍了三维及二维微凝胶胶体晶体组装的研究进展,并对已开发的基于微凝胶胶体晶体的应用进行了总结.     

Preparation of non-contact ordered array of polystyrene colloidal particles by using a metallic thin film of fused hemispheres

A thin metallic bilayer consists of fused hollow hemispheres of 930 nm in diameter is fabricated by sputter deposition of Ti and Fe at 50 and 5 nm of thickness, respectively, onto an array of spherical polystyrene colloidal particles. The fused metal hemispheres are utilized to assemble polystyrene colloidal particles of smaller diameters (800 nm) into non-contact two-dimensional periodic array by trapping them in the metallic wells.