球型胶体颗粒的表面电位和表面电荷密度的关系

胶体颗粒的表面电荷密度和表面电位之间的关系是颗粒表面的基本性质之一．要确定这个关系,需要解Poisson-Boltzmann(PB)方程,求出颗粒外的电位分布．然而对于球形颗粒,PB方程却没有解析解．Loeb等,求出了数值解,近似解析表达式虽然很多,也比较复杂,     

流动电位/胶体滴定法测定聚电解质电荷密度的研究

探讨了应用粒子电荷测定仪的流动电位判定胶体滴定终点的可行性。结果表明流动电位曲线能在样品浓度大于 0 .6× 1 0 - 5mol· L- 1的溶液中准确指示胶体滴定的终点 ,较常用指示剂邻甲胺兰的使用极限浓度低一个数量级。观察到由阳离子聚电质滴定阴离子聚电质能减少盐干扰的现象。叔胺型阳离子淀粉应在酸性下滴定     

单分散表面带正电荷聚苯乙烯胶体粒子的制备及胶体晶体阵列的构筑

以苯乙烯为单体,甲基丙烯酰氧乙基-N-辛基二甲基溴化铵为功能单体,偶氮二异丁基脒盐酸盐为引发剂,采用两步投料无皂乳液聚合方法,合成了单分散表面带正电荷的聚苯乙烯胶体粒子。在低离子强度的水溶液中,该胶体粒子可以通过表面电荷的静电排斥作用,自组装成胶体晶体阵列并产生Bragg衍射,随着乳液固含量的降低,Bragg衍射波长红移。     

带电悬浮粒子胶体晶体的固定化

采用光固化技术, 以丙烯酰胺单体与亚甲基双丙烯酰胺交联剂在紫外光的照射下发生光聚合反应, 嵌入聚苯乙烯胶体晶体, 实现了胶体晶体的固定化. 结合反射光谱和Kossel衍射技术研究对照了固定化前后胶体晶体的变化, 实验结果表明, 通过这种水凝胶固定化的胶体晶体保存了未固定前悬浮液中胶体晶体的结构. 但固定化后的胶体晶体的晶面间距和晶体的尺寸都略微减小. 通过对固定化后的水凝胶长时间的反射光谱观测, 发现固定化后胶体晶体在Milli-Q水中起初会发生溶胀, 经过2-5天溶胀-消溶胀过程达到平衡, 平衡后的水凝胶胶体晶体十分稳定, 可以长时间保持胶体晶体的结构. 因此, 胶体晶体固定化不但极大地提高了悬浮液中胶体晶体的抗剪切能力, 还克服了悬浮液中胶体晶体对离子、外界干扰的敏感性, 扩大了胶体晶体的实际应用价值.     

胶体刻蚀——纳米结构化表面的构筑与应用

综述了近年来胶体刻蚀领域的研究进展, 分别讨论了基于胶体微粒和胶体晶体为模板的可控沉积与可控刻蚀及在固体平面基质、曲面基质和气液界面等不同基质上构筑结构化表面的方法. 同时还探讨了利用胶体刻蚀方法形成的微纳结构在光、电、磁以及表面润湿和生物学等方面的应用.     

熵驱大分子胶体粒子的柱状受限结晶

<正>熵是物理化学的基本状态参量,在统计力学和热力学中处于核心位置.按照玻尔兹曼的微观解释,熵可以由孤立系统微观状态的数目(W)给出,即S=k_BlnW,这里k_B为玻尔兹曼常数^[1,2].根据此公式,微观状态数越多,系统越混乱,熵越大,所以熵常被视作体系无序程度的度量.但熵增仅对应体系微观     

基于温敏水凝胶的可调胶体晶体制备

基于单分散胶体粒子悬浊液在温敏水凝胶表面可以形成湿润型胶体晶体的现象, 利用温敏水凝胶对水的控释作用制备了温度敏感的可调制胶体晶体. 在室温下利用提拉法在温敏水凝胶聚N-异丙基丙烯酰胺(PNIPAAm)表面制备湿润型胶体晶体膜. 由于胶体粒子的有序排列, 胶体晶体显示出一个尖锐的反射峰. 当温度上升到34 ℃以上时, 由于PNIPAAm水凝胶中的水被释放, 导致胶体晶体中粒子浓度降低, 粒子间距增加; 反射峰发生红移. 这些特性可以通过温度变化进行调制.     

双电层相互作用时胶体表面电位的分布及电荷密度的计算

本文以实验为基础,运用计算机数值解解出双电层相互作用时平面胶体表面电位ψ随距离X的分布,依据作者导出的双电层相互作用时胶体表面阴离子负吸附方程,计算出胶体表面外Hclmhotz面(OHP)处的表面电荷密度σ_δ;讨论了双电层相互作用程度(ψ_d/ψ_δ)对胶体表面电位分布及其表面电荷密度的影响。     

胶体粒子的机械性能调控及其在药物递送中的应用

胶体粒子是肿瘤治疗中最常用的载体, 尽管在过去的研究中不同的胶体粒子已经被广泛报道, 但如何进一步提高胶体粒子的药物递送效率仍然存在着一些挑战. 大量的研究表明胶体粒子的尺寸、形状、结构和表面化学等物理化学性质在药物递送过程中具有重要的作用, 但胶体粒子的机械性能对药物递送过程的影响研究和综述相对较少. 本综述从不同机械性能胶体粒子的制备与表征出发, 概述了胶体粒子的机械性能对血液循环、肿瘤富集、渗透以及细胞内化过程的影响, 并对该领域存在的问题以及发展的趋势进行了展望. 该综述有助于帮助科学工作者更好地理解胶体粒子的机械性能对药物递送的影响规律, 从而优化胶体粒子的设计并提高纳米药物的递送效率和生物利用率.     

胶体晶体自组装排列进展

自组装排列胶体晶体是发展光子晶体等亚微米周期有序结构及新型光电子器件十分重要的环节.高电荷密度单分散胶体球在较弱的离子强度和稀浓度下会自发排列形成紧密堆积的周期性结构(ccp),常常是面心立方(fcc),科学家们以此为基础发展了多种结晶化胶体粒子的方法,包括重力场沉积、电泳沉积、胶体外延技术、垂直沉积、流通池、物理束缚排列及其他的许多方法.目前排列的胶体粒子基本为球形,材料也多为SiO2、PS、PMMA,此外一些复合粒子,主要为核壳粒子的排列这里也稍作介绍,这些方法及其变通的使用可以形成类蛋白石及反蛋白石结构,最终实现光子带隙及其它多种用途。     

Influence of Sedimentation on Crystallization of Charged Colloidal Particles

The method of density matching between the solid and liquid phases is often adopted to effectively eliminate the effect of sedimentation of suspensions on dynamic behavior of a colloidal system. Experiments on crystallization of charged colloidal microspheres with di-ameter of 98 nm dispersed in density-matched and -unmatched media (mixtures of H₂O and D₂O in proper proportion) are compared to examine the influence of sedimentation. Reflection spectra of colloidal suspensions were used to monitor the crystallization process. Results showed that the crystal size of the density-unmatched (namely, in the presence of sedimentation) sample grew faster than that of the density-matched (in the absence of sedi-mentation) case at the initial stage of the crystallization, and then the latter overtook and outstripped the former. To explain these observations, we assume that in the settling of crystals sedimentation facilitates result in more particles getting into the crystal structures. However, as the crystals increase to varying sizes, the settling velocities become large and hydrodynamic friction strips off some particles from the delicate crystal structures. Overall, the sedimentation appears to accelerate the crystal size growth initially and then retard the growth. In addition, the crystal structures formed under microgravity were more closely packed than that in normal gravity.     

Effect of Charge,Size and Temperature on Stability of Charged Colloidal Nano Particles

Molecular simulation of charged colloidal suspension is performed in NVT canonical ensemble using Monte Carlo method and primitive model. The well-known Derjaguin-Landau-Verwey-Overbeek theory is applied to account for effective interactions between particles. Effect of temperature, valance of micro-ions and the size of colloidal particles on the phase stability of the solution is investigated. The results indicate that the suspension is more stable at higher temperatures. On the other hand, for a more stable suspension to exist, lower micro-ion valance is favorable. For micro-ions of higher charge the number of aggregates and the number of particle in each of aggregate on average is higher. However for the best of our results larger colloidal particle are less stable. Comparing the results with theoretical formula considering the influence of surface curvature shows qualitative consistency.     

高电位胶体颗粒强相互作用的近似表达式

When surface potential of the particles, ,is high,sinh y can be approximated by ≈ey/2 in the nonlinear Poisson Boltzmann equation.Thus,we present a simple method of calculating the interaction force and energy per unit area between two dissimilar plates with high potentials at constant surface potential.These formulae could be applicable to the case of repulsive case,in which the derivative of y must vanish at an interior point,and a minimum ymin=u always exists.A turning point at ～kh≈2(1)e－y1/2 for the repulsion or attraction between dissimilar planar surfaces.These formulae are divergent at 阧∞,and zero point at kh≈2 .This means that they can only be used at 阧 < 2 and accurate location is at kh ≤ 4. 　　Agreement of the approximation for force,Eq.（13）,is good with the exact numerical values of the interaction of dissimilar plates given by Devereux [6] for high surface potentials.For y1 ≥5 kh ≤ 3.0 the relative errors of Eq.(13) are less than 5％,and for kh ≤ 3.5 relative errors are less than 10％.For the interaction energy,Eq.(15),the applicable range extends to kh =4.0.Beyond this range the error increases rapidly.The higher surface potential is the better the precision of Eq.（13）and Eq.( 15).The condition of the strong interaction has been satisfied.     

Colloidal crystals of cationic spheres

Colloidal single crystals of cationic polymer spheres (198–250 nm in diameter) in deionized aqueous dispersions were formed for the first time. The spheres used were poly(styrene-co-methacryloyloxyphenyldimethylsulfonium) cations. These cations are unstable in deionized suspensions with mixed beds of cation-exchange and anion-exchange resins. This was clarified by reflection spectroscopy, pH, conductance and -potential measurements for 250 days after suspension preparation. Colloidal crystals formed over a period of 24 h for the deionized suspensions at sphere concentrations higher than 0.09 in volume fraction. The nearest-neighbor intersphere distances coincide satisfactorily with the calculated values using the diameter and the concentration of the spheres. Alloy crystals formed from binary mixtures of the cationic polymer spheres and the anionic silica spheres when the ratio of the volume fraction of cationic spheres against the sum of the both cationic and anionic spheres was smaller than 0.3.     

Interdigitated Conductometric Immunosensor for Determination of Interleukin‐6 in Humans Based on Dendrimer G4 and Colloidal Gold Modified Composite Film

A highly sensitive, fast and stable conductometric immunosensor for determination of interleukin‐6 (IL6) in humans is developed by encapsulation of horseradish peroxidase‐labeled interleukin‐6 antibody (HRP‐anti‐IL6) in poly(amidoamine) fourth‐generation dendrimer (dendrimer) and colloidal gold (nanogold) modified composite architecture. The presences of nanogold and dendrimer provided a congenial microenvironment for the immobilized biomolecules and decreased the electron transfer impedance, leading to a direct electrochemical behavior of the immobilized HRP. The formation of the antibody‐antigen complex by a simple one‐step immunoreaction between the immobilized HRP‐anti‐IL6 and IL6 in sample solution introduced a barrier of direct electrical communication between the immobilized HRP and the gold electrode surface, thus local conductivity variations could be detected by the HRP electrocatalytic reaction in 0.02 M phosphate buffer solution (pH 7.0) containing 50 μM H₂O₂, 0.01 M KI and 0.15 M NaC1. Under optimal conditions, the proposed immunosensor exhibited a good conductometric response to IL6 in a linear range from 30 to 300 pg/mL with a relatively low detection limit of 10 pg/mL at 3δ. The precision and reproducibility are acceptable with the intra‐assay CV of 7.3% and 5.6% at 100 and 200 pg/mL IL6, respectively. The storage stability of the proposed immunosensor is acceptable in a pH 7.0 PBS at 4 °C for 8 days. Importantly, the proposed methodology could be extended to the detection of other antigens or biocompounds.     

Microwave-Assisted Self-Organization of Colloidal Particles Inside Water-in-Oil Emulsions

Commercial amidine polystyrene microspheres were self-organized to obtain colloidal microclusters from water-in-oil emulsion droplets as confining geometries. For demulsification process, microwave was irradiated to remove water droplets selectively resulting in the shrinkage of water droplets which induces inward capillary pressure for the particle self-assembly. The amidine polystyrene clusters were coated with silica nanospheres or titania nanoparticles by co-organizing the mixed particle suspensions inside water droplets by microwave heating. Titania-coated polystyrene clusters were calcined to produce hollow macroporous titania powders. Finally, sulfate-coated polystyrene microspheres were self-assembled with silica nanoparticles to generate polystyrene/silica composite clusters by microwave irradiation method.     

电导滴定法对苯乙烯/丙烯酸无皂乳液共聚微球表面性质的研究

本文主要叙述用电导滴定法对羧化微球表面的羧基含量进行了测定,以便了解其表面特性与IgG吸附的关系,进而获得满意的微球产品。     

聚苯乙烯胶态晶体的合成

近年来 ,胶态晶体引起物理学家和化学家的共同关注 [1] .占据晶格点的纳米或微米级微粒自组装行为 [2 ] 在光学显微镜和扫描电子显微镜下可被清晰地观察到 ,因此能作为研究晶体相变的模型 [3 ] ,并有助于人们加深对晶体中点缺陷、晶界及位错等现象的了解 .胶态晶体所具有的周期性结构更使其在光学研究领域具有特殊意义 .与半导体中电子的能带结构类似 [4 ] ,胶态晶体中传播的光波色散曲线为不连续的带状结构 ,被称为“光子晶体”(photonic crystal) .在禁带区 (photonic band gap) ,光被禁止传播 ,而光散射加强 ,可将其应用于光电开关及光催…