分散体系中任意形状的胶粒模型与相互作用能——Ⅱ、不等同球颗粒

鉴于不等同球颗粒在胶体化学中的重要性,所以它一直引起人们在理论上的关注。Hogg、Healy和Fuerstenau(HHF)对Poisson-Boltzmann方程引用Debye-Hückl近似,得出不同平行平板型颗粒在恒电位表面时相互作用能计算公式,进而HHF用Derjaguin法得出不等同球颗粒相互作用能的表达式。虽然HHF的公式仅适用低电位的情况,但它的表达式特别简单,因而一直被广泛使用。Ohshima等(OCHW)对球颗粒做了曲率校正,Barouch等(BM)对Poisson-Boltzmann方程提出二维解法,使不等同球颗粒的相互作用能的计算有了改进和提高。本文根据我们提出的模型和方法,对HHF公式也做了曲率校正,结果表明它和OCHW的曲率校正结果相当,但它的表达式却要简单得多。     

泛函迭代法研究等同平行平板双电层间的相互作用

利用泛函分析理论中的迭代法, 分别计算了等同平行平板双电层在128、77、和25 mV电位下的相互作用能. 并以数值法所得结果为参照, 在各电位下分别与Debye-Huckel(DH)线性近似法、Langmuir 近似法所得的结果进行比较. 结果表明, DH线性近似法和Langmuir近似法均只能分别局限于极低或极高电位, 而泛函迭代法不但有简单的解析表达式, 而且在各种电位下都能得到较满意的结果.     

颗粒模板法制备大孔Al2O3材料

采用颗粒模板法制备了大孔氧化铝(Al2O3)材料. 扫描电子显微镜(SEM)结果显示, 大孔Al2O3结构中的大孔呈“囊泡状”且孔道的贯通性较差. Zeta电位测量表明, 共沉积条件下聚苯乙烯(PS)和Al2O3两种胶体颗粒带有相反的电荷, 在静电引力作用下先发生了吸附, 再沉积在一起. 吸附在PS微球表面的Al2O3纳米颗粒形成的吸附层是导致大孔呈“囊泡状”和孔道不贯通的主要原因. 采用聚二烯丙基二甲基氯化铵(PD)溶液对PS胶体微球带电性质进行了改性, PS微球的Zeta电位由−44.36 mV变成了+37.41 mV, 进而消除了沉积过程中二元颗粒间的吸附现象. 扫描电子显微镜显示, 大孔样品中“囊泡状”大孔消失, 同时孔道贯通性得到改善.     

球型胶粒间的相互作用能—Derjaguin法的改进

对求算球型胶体颗粒相互作用能的Ｄｅｒｊａｇｕｉｎ法进行了适当的修正，并由此得出简单的解析表达式，对低电位条件下等同和不等同球颗粒的计算结果表明，该法拓宽了Ｄｅｒｊａｇｕｉｎ公式的应用范围，提高了计算结果的精确度。     

种子乳胶粒表面修饰法制备核壳结构PSt/TiO_2复合微球

首先采用无皂乳液聚合法合成了表面带负电荷、粒径为360 nm的单分散聚苯乙烯(PSt)乳液,并利用聚乙烯亚胺(PEI)在25℃下对PSt乳胶粒表面进行修饰,得到了表面带有正电荷的PSt种子乳液;然后以乙醇和水的混合物为反应介质,采用种子乳液加入法,使钛酸正丁酯(TBT)在修饰后的乳胶粒表面进行水解与缩合,制备出了核壳结构PSt/TiO2复合微球,利用电镜对复合微球的结构形态进行了表征.结果表明,PSt乳液改性时体系的zeta电位随着PEI用量的增加而升高,当PEI用量为PSt聚合物重量的15%时,体系的zeta电位从原来的-40.3 mV升高到了38.3 mV,达到对PSt乳胶粒表面改性的最佳值;在制备PSt/TiO2复合微球时,TiO2包覆量随着反应时间的延长而增加,反应7 h时达到90.2%的最大值;随介质中水含量的增加,吸附到复合微球表面上的TiO2纳米颗粒逐渐减少,复合微球表面逐渐变得光滑,当EtOH/H2O质量比为100/6.0时,得到结构均一、壳层厚度为29 nm的核壳结构PSt/TiO2复合微球.     

碳球担载二硫化钴纳米复合电催化剂的制备及其析氢性能研究

采用一步水热法,通过引入载体碳球(CSs)和表面活性剂CTAB,将二硫化钴(CoS_2)纳米颗粒均匀负载在CSs表面.相比于单独的CoS_2,改性后CSs担载的CoS_2(CoS_2/A-CSs)展现出了更好的电催化活性.在电解液为0.5mol/L H_2SO_4溶液中,电流密度为10 mA·cm~(-2)条件下,其析氢反应过电位仅为154 mV.经过12 h的稳定性测试,CoS_2/A-CSs析氢反应过电位为180 mV,这表明其仍具有良好的电化学催化析氢反应活性.这种复合电催化剂的优良性能主要归因于CSs的高导电性和其对CoS_2纳米颗粒的均匀分散;此外,CTAB的引入,促使CSs与CoS_2之间结合的更加紧密,进而加快了活性位点间的电子传导.     

种子表面改性法制备核壳结构PSt/SiO_2复合微球

首先采用无皂乳液聚合法合成了表面带负电荷、粒径为360nm的单分散聚苯乙烯(PSt)种子乳液,并以EtOH/H2O混合物为分散介质,利用γ-氨丙基三乙氧基硅烷(KH-550)在25℃下对PSt微球表面进行改性,得到了表面硅烷化并带有正电荷的改性PSt种子乳液,然后在碱性条件下加入原硅酸乙酯(TEOS)使其和微球进行共水解与共缩聚,制备出了核壳结构PSt/SiO2复合微球,并利用电镜对复合微球的结构形态进行了表征.研究表明,PSt种子乳液改性时体系的zeta电位随着KH-550用量的增加而升高,当KH-550用量为PSt种子重量的1/3时,体系的zeta电位从原来的-34.5mV升高到了38mV,达到对PSt微球表面改性的最佳值;在制备PSt/SiO2复合微球时,TEOS水解缩聚形成的SiO2包覆到改性微球上的量随着反应时间的延长而增加,反应24h时达到97.9%的最大值;随介质中水含量的增加,吸附到复合微球表面上的SiO2纳米颗粒逐渐减少,复合微球表面逐渐变得光滑,当EtOH/H2O质量比降低到60/28.5时,得到结构均一、壳层厚度为35nm的核壳结构PSt/SiO2复合微球。     

壳聚糖修饰PLGA阳离子型纳米微球的制备与表征

采用单乳化-溶剂(O/W)挥发技术制备表面带正电荷的壳聚糖(CHS)修饰聚乙/丙交酯(PLGA)纳米微球(PLGA/CHS), 通过正交试验优化了纳米微球的制备条件. 结果表明, 微球粒径可控制在150～200 nm内, 在pH=4时, 纳米微球表面电位最高为55 mV. 影响微球粒径的主要因素是聚合物的浓度, CHS的分子量和浓度以及介质的pH值对微球表面电位也有明显影响. 制备粒径较小而表面电位较高的PLGA/CHS纳米微球条件为: ρ(CHS)=3 mg/mL, ρ(PLGA)=10 mg/mL, Vo/Va=1/4. SEM图像显示经CHS修饰的PLGA的纳米微球形状规整, 荧光显微观察和XPS分析结果证实CHS包覆于微球表面.     

双敏性微凝胶的絮凝及聚沉行为

用沉降聚合法制备了聚(N-异丙基丙烯酰胺-co-甲基丙烯酸)微凝胶, 并用NMR, DLS分析测定了微凝胶结构及凝胶颗粒在不同离子强度下粒径和表面电势的变化. 25 ℃时在pH＝7的溶液中Zeta电位为－18 mV, 随离子强度增加, 逐渐减小. 当NaCl浓度达0.2 mol/L时基本不变, 表明微凝胶表面电荷受到屏蔽, 浓度继续增加主要使凝胶颗粒收缩. 加热引起微凝胶收缩, 颗粒表面电荷密度增大, Zeta电位增大. 在0.2 mol/L NaCl溶液中, 41 ℃时微凝胶的Zeta电位可达－12.4 mV, 使微凝胶稳定. 较高离子强度时, Zeta电位随温度升高发生突变, 微凝胶表面几乎为中性, 其突变温度与临界絮凝温度(CFT)相当. CFT随离子强度增加向低温迁移, 微凝胶聚集速率在高温时比低温时快.     

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,     

球胶体颗粒之间相互作用能的求解

根据线性迭加近似方法,定义了一个修正电位项,较详细地推导出用于中等电位条件下球形胶体颗粒相互作用能和力的公式,该公式较为简单、实用,然而,对其所做的改进主要是针对相互作用能而不是力,对其原因也作了简单的讨论.     

Improvement on the Derjaguin's method for the interaction of spherical particles

A correction to the classical Derjaguin's method has been given for the electrical double layer interaction of two spherical particles. Simple analytic expressions are given. Results obtained respectively for identical and dissimilar spherical particles show that the expressions open up the usable area of familiar Derjaguin's formulas.     

The response of a colloidal suspension to an alternating electric field

This paper is concerned with the calculation of the complex conductivity K* of a suspension, a quantity which may be determined experimentally from the measurement of the alternating current which flows between a pair of electrodes in the suspension due to an alternating voltage difference. A semi-analytic formula is derived for the complex conductivity of a dilute suspension of spherical particles with small dielectric constant which is reasonably accurate for ?-potentials of less than 50 mV. For such suspensions this formula represents a very economical alternative to the exact computer calculation of K* described by DeLacey and White (ref. 2). Although the formula for K* is derived for particles with fixed surface charge, it is shown that the formula can also be applied to a more general class of suspensions, in which the surface charge arises from the dissociation of a single type of surface group.     

Approximate expressions of determining the double layer energy and force of interaction between two charged colloidal spheres

The approximate expressions have been obtained to calculate the electrical double layer energy and force between two spherical colloidal particles based on the improved Derjaguin approximation. Results for identical spheres interacting under constant surface potential, constant surface charge are given. Comparison of present results with numerical results calculated by Carnie and Chan is made. The expressions are found to work quite well for the constant surface potential case, and for the constant charge case, we make correction for the expressions. The results given are satisfactory providedkh0.4.     

Electrophoresis of a charge-regulated sphere at an arbitrary position in a charged spherical cavity

The electrophoresis of a charge-regulated spherical particle at an arbitrary position in a charged spherical cavity is modeled under conditions of low surface potential (<25 mV) and weak applied electric field (<25 kV/m). The charged cavity allows us to simulate the effect of electroosmotic flow, and the charge-regulated nature of the particle permits us to model various types of surface. The problem studied previously is reanalyzed based on a more rigorous electric force formula. In particular, the influences of various types of charged conditions on the electrophoretic behavior of a particle and the roles of all the relevant forces acting on the particle are examined in detail. Several new results are found. For instance, the mobility of a particle has a local minimum as the thickness of a double layer varies, which is not seen in the cases where the surface of a particle is maintained at a constant potential and at a constant charge density.     

Heterocoagulation in Bidisperse Magnetorheological Fluids Containing Like-Charged Nanosized and Micron Particles Without a Magnetic Field

Based on extended Derjaguin–Landau–Verwey–Overbeek theory, a heterocoagulation model is proposed for magnetorheological (MR) fluids containing like-charged nanosized and micron particles without a magnetic field. This model considers three major interactions, namely van der Waals attraction, electrical double layer (EDL) interaction, and steric repulsion. The EDL interaction has been identified as the most important factor. The surface potential ratio β (ψ₂/ψ₁) between two dissimilar particles with like charge plays an important role in controlling the change of EDL interaction. At higher β ratios, the EDL interaction becomes attractive when the surface separation falls within a certain range. Two groups of MR fluid samples have been used in experimental studies based on electroacoustic measurements. In the first group, the ratio and the sum of the zeta potentials between carbonyl iron particles and ceria were 4 and ?734.57 mV, respectively. In the second group, these parameters were 1.38 and ?108.17 mV, respectively. The experimental results suggested that the second group did not undergo heterocoagulation, whereas the first group showed extensive heterocoagulation. The difference in surface potentials between particles of two different phases has been found to be critical for determining the state of dispersion or heterocoagulation in concentrated MR fluid systems.     

Simple Approximate Expressions for Electrical Double-Layer Interaction at Constant Moderate Potentials

Simple yet accurate expressions for the electrical double-layer interaction force and energy between the particles that hold for a wide range of surface potential is required in the modeling, simulation, and optimization of many processes employed in industry. In this paper, simple approximate expressions for the interaction are obtained based on the asymptotic results and the numerical solution to the Poisson-Boltzmann equation for identical parallel plates with constant surface potential up to 180/z(i) mV at 25 degrees C, and the Derjaguin approximation. Within the moderate surface potential range, the semianalytical expressions agree well with the exact numerical results and are convenient to use for the purpose of process modeling and simulation. Copyright 2000 Academic Press.     

分散体系中任意形状的胶粒模型与相互作用能——Ⅰ. 相同的球颗粒

本文提出了一种计算任意形状胶粒相互作用的新方法。把粒胶做为一个凸面体, 做出它的支持平面, 当假定两凸面体的支持平面之间的排斥能可以由经典DLVO理论计算时, 令一凸面体(或它的相似体)沿另一凸面体(或它的相似体)转动, 那么, 两凸面体胶粒之间的排斥能, 就是支持平面之间的排斥能沿凸面体(或它的相似体)的表面积分。计算结果表明, 这种方法十分简便, 又有足够高的精确度。     

Sedimentation Velocity and Potential in Concentrated Suspensions of Charged Spheres with Arbitrary Double-Layer Thickness

The sedimentation in a homogeneous suspension of charged spherical particles with an arbitrary thickness of the electric double layers is analytically studied. The effects of particle interactions are taken into account by employing a unit cell model. Overlap of the double layers of adjacent particles is allowed, and the polarization effect in the double layer surrounding each particle is considered. The electrokinetic equations that govern the ionic concentration distributions, the electric potential profile, and the fluid flow field in the electrolyte solution in a unit cell are linearized assuming that the system is only slightly distorted from equilibrium. Using a perturbation method, these linearized equations are solved for a symmetrically charged electrolyte with the surface charge density (or zeta potential) of the particle as the small perturbation parameter. An analytical expression for the settling velocity of the charged sphere in closed form is obtained from a balance among its gravitational, electrostatic, and hydrodynamic forces. A closed-form formula for the sedimentation potential in a suspension of identical charged spheres is also derived by using the requirement of zero net electric current. Our results demonstrate that the effects of overlapping double layers are quite significant, even for the case of thin double layers. Copyright 2000 Academic Press.