重氮树脂—聚磷酸复合物

带有相反电荷 (通常在侧链 )的聚电解质 ,通过静电相互作用形成的复合物 ,称聚电解质复合物 (ＰＥＣ) .ＰＥＣ已有很多研究[1～ 3] ,也有一些应用的报道[4,5] .重氮树脂 (ＤＲ) ,一种由二苯胺 4 重氮盐与多聚甲醛在浓硫酸中缩合得到的缩聚物[6] ,因侧链带重氮基 ,所以是正离子聚电解质 .它能与各种负离子聚电解质生成感光性的ＰＥＣ ,并可用作光成像体系的感光剂[7,8] .ＤＲ与聚磷酸 (ＰＰＡ)生成重氮基为正离子 ,磷酸基为负离子的复合物 ,这种复合物文献上未有过报道 .本文初步研究了这种复合物的制备与性质 .1　重氮树脂 聚磷酸复合物 (…     

聚电解质混合物在均匀带电平面上吸附的密度泛函研究

采用非局域密度泛函理论计算方法(NLDFT), 我们研究了两种带相反电荷的聚电解质混合物在均匀带电平面上的吸附以及吸附层的电荷反转现象. 我们对表面带电密度和聚电解质链段的价态对吸附的影响做了系统研究, 发现在体系中不含小离子的情况下, 当体系中两种聚电解质链段都为单价时, 和表面带相反电荷的聚电解质链能够吸附在平面上, 而和表面带相同电荷的聚电解质链和表面之间相互排斥, 整个过程就是表面电荷被与之带相反电荷的聚电解质链上所带电荷中和的过程, 没有出现明显的电荷反转现象|当体系中作为反离子存在的聚电解质链段价态为二价时, 和表面带相同电荷的聚电解质链能在表面上吸附, 出现明显的电荷反转现象. 理论研究表明, 以反离子居中为媒介的静电相关效应是聚电解质混合物出现多层吸附的主要驱动力之一.     

聚电解质溶液热力学性质的研究

本文采用柱形胞腔模型以及Vink的近似方法, 求解聚电解质溶液的Poisson-Boltzmann方程, 得到不同条件下聚离子周围静电势的分布。进而得到了不同条件下聚离子、反离子和同电荷离子的活度系数及溶剂的渗透系数。所得结果与实验值能较好地吻合。     

聚电解质复合物在表面活性剂水溶液中的溶解机理

聚电解质复合物 ( PEC)因其独特的物理化学性质而受到广泛关注 .对其研究主要集中在其结构及形成的影响因素 ,如聚电解质的分子量 [1,2 ] 、电荷密度、电荷强弱 [1,2 ] 及溶液离子强度 [3,4 ] ,而很少有关于聚电解质复合物溶解性的报道 [5,6 ] .一般认为组成 PEC的聚正离子 ( PC)和聚负离子 ( PA)之间 ,通过离子键形成网状交联结构而不溶于水及有机溶剂 .只有一种特殊的溶剂体系屏蔽溶剂可溶解此类复合物[7,8] .本文报道一类新的聚电解质复合物 :以二苯胺重氮树脂 DR为聚正离子 ,苯乙烯 -马来酸酐碱性水解物 ( PSMNa)为聚负离子的 P…     

旋光聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸]的合成及静电自组装

以聚(乙烯-alt-马来酸酐)为原料,通过与R-(+)-α-苯乙胺的酰胺化反应,合成了一种新型的旋光聚电解质聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸],利用红外吸收光谱、紫外吸收光谱、核磁共振氢谱和旋光度数据对其结构进行表征.聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸]与聚二甲基二烯丙基氯化铵(PDDA)逐层静电自组装过程的紫外跟踪测试结果表明,带相反电荷的聚电解质间能够形成稳定增长的自组装膜,多层膜组装量随双层数指数增大.     

高价盐对柱状聚电解质刷的效应

应用标度理论研究了外加的高价反离子对柱状聚电解质刷的影响.以外加盐浓度的不同,在单价盐情况下,强和弱聚电解质刷分别有2个和3个标度区域,而在高价盐情况下,柱状聚电解质刷的行为可分为4个区域.第一个区域,盐浓度很低,刷的行为不依赖于外加盐浓度.第二个区域,外加盐浓度对刷的行为开始有影响,刷的厚度随外加盐浓度增大而减小.第三个区域,强聚电解质刷厚度不依赖于外加盐浓度,而弱聚电解质刷厚度反而随外加盐浓度增大而升高.第四个区域,聚电解质刷厚度随外加盐浓度升高而降低,行为类似单价盐情形下的盐刷.这些区域都是链熵弹性与小离子渗透压平衡造成的,与单价和高价反离子在刷内的交换密切相关.新发现的区域尚待实验和计算机模拟的验证.     

壳聚糖与重氮树脂磺酸盐的感光性超薄膜

由于壳聚糖 ( CS)具有抗菌性、抗病毒性、良好的生物相容性、生物降解性以及容易与金属离子螯合等性质 ,被广泛用于重金属回收 [1～ 3] 、药物释放 [4～ 6] 、伤口覆盖[7,8] 、膜分离 [9,10 ] 、日用化工 [11] 等方面 .近年来 ,人们对壳聚糖以及它的化学改性作了大量的研究 [12～ 14 ] .其中通过化学改性形成壳聚糖聚电解质 ,可与带相反电荷的聚电解质通过静电自组装 ( ESA)获得超薄膜 [15～ 18] .本文尝试用壳聚糖( CS)与二苯胺 - 4-重氮树脂磺酸盐 ( DRS)以及二苯胺 - 4-重氮树脂 ( DR)通过 ESA的方法 ,形成具有感光性的超薄膜 .经 …     

金电极表面植物原生质体的固定化

近年来 ,基于聚电解质同携带相反电荷的基团之间的静电吸引作用组装超薄复合膜的研究受到广泛的关注 [1～ 7] .但是 ,利用聚电解质来固定生物活细胞的研究尚不多见 .Wen等 [8]曾在水溶液中利用聚电解质复合物构成的微囊来固定人体肿瘤活细胞 .本文将该技术应用于生物活细胞在电极表面的固定化 .利用吸附在金电极上的荷正电的聚二烯丙基二甲基氯化铵 [Poly( diallyldimethylammoniumchloride) ,PDADMAC]将携带负电荷的大麦细胞固定在金电极表面 ,运用扫描隧道显微镜 ( STM)、石英晶体微天平 ( QCM)及共焦激光扫描荧光显微镜对该过程进…     

微孔型固体偏氟乙烯-六氟丙烯共聚物电解质

将固体聚合物电解质 (Ｓｏｌｉｄｐｏｌｙｍｅｒｅｌｅｃｔｒｏｌｙｔｅ)用于锂离子电池的研究已经有 3 0年的历史[1] ,从物理角度来看 ,研究过干态型 (ＤｒｙＳＰＥ)、凝胶型 (ＧｅｌｌｅｄＳＰＥ)和微孔型固体聚合物电解质 (ＰｏｒｏｕｓＳＰＥ)三大类型[2 ] ;从化学角度来看 ,研究过含氧、含氮、和含氟的等聚合物[1～ 6 ] .微孔型固体含氟聚合物电解质是近 1 0年来才开始研究并受到产业界很大关注的一种ＳＰＥ .固体聚合物电解质的应用可以解决液体电解质锂离子电池的漏液问题 ,并提高其安全性 ,还可以通过使用塑料包装来减小电池的重量…     

粘度法测定部分水解聚丙烯酰胺的分子量

在 2 5℃、浓度为 1mol L的NaCl水溶液中 ,测定了聚合度 (DP)为 1 48× 10 3～ 3 79× 10 4的聚丙烯酰胺 (PAM)及其水解度 (h)在 0 %～ 70 %之间的部份水解聚丙烯酰胺 (HPAM)的特性粘度 ([η]) .根据聚电解质理论和Kowblansky的研究结果 ,建立了特性粘度 [η]与聚合度DP、水解度h之间的定量关系式 :[η]=0 1113DP0 83 2 9+0 9973DP0 753 1 (1- 0 81h1 2 )h .用该式处理方献数据 ,其平均误差为 13 74%     

pePC-SAFT: Modeling of polyelectrolyte systems: 1. Vapor–liquid equilibria

A molecular thermodynamic model for polyelectrolyte systems—called pePC-SAFT—is proposed. The effect of charged monomers within the polyelectrolyte chain is explicitly taken into account in the reference term by replacing the hard-chain contribution of the PC-SAFT model by a charged-hard-chain contribution. Moreover, counterion condensation is accounted for to determine the effective number of charges along the polyion as well as of free counterions. The electrostatic contribution of the free counterions is described by a Debye–Hückel term.     

Density functional theory for planar electric double layers: closing the gap between simple and polyelectrolytes

We report a nonlocal density functional theory (NLDFT) for polyelectrolyte solutions within the primitive model; i.e., the solvent is represented by a continuous dielectric medium, and the small ions and polyions by single and tangentially connected charged hard spheres, respectively. The excess Helmholtz energy functional is derived from a modified fundamental measure theory for hard-sphere repulsion, an extended first-order thermodynamic perturbation theory for chain connectivity, and a quadratic functional Taylor expansion for electrostatic correlations. With the direct and cavity correlation functions of the corresponding monomeric systems as inputs, the NLDFT predicts the segment-level microscopic structures and adsorption isotherms of polyelectrolytes at oppositely charged surfaces in good agreement with molecular simulations. In particular, it faithfully reproduces the layering structures of polyions, charge inversion, and overcharging that cannot be captured by alternative methods including the polyelectrolyte Poisson-Boltzmann equation and an earlier version of DFT. The NLDFT has also been used to investigate the influences of the small ion valence, polyion chain length, and size disparity between polyion segments and counterions on the microscopic structure, mean electrostatic potential, and overcharging in planar electric double layers containing polyelectrolytes.     

Distribution of counterions in the double layer around a cylindrical polyion

The modified Poisson-Boltzmann (MPB) equation, and the Monte Carlo (MC) method, were applied to the cell model of a polyelectrolyte solution in order to calculate the distribution of counterions around a cylindrical polyion. Both methods suggest stronger binding of counterions to the polyion than predicted by the ordinary Poisson-Boltzmann (PB) equation. The inclusion of counterion-counterion correlation being neglected in the PB equation, leads to a better agreement of the calculated osmotic coefficients with those measured.     

两性聚电解质溶液的分子热力学模型和分子动力学模拟

从带电硬球混合物出发采用化学缔合理论建立了聚电解质和两性聚电解质溶液的分子热力学模型.用考虑溶剂的粘滞力和热浴随机力作用的分子动力学(MD)方法模拟了聚电解质和两性聚电解质溶液的渗透系数.对模型预测结果和MD模拟结果进行了比较,表明基于化学缔合理论的分子热力学模型可以用于聚电解质溶液和两性聚电解质溶液热力学性质的预测,对于均聚电解质溶液效果令人满意,对由直径不同的离子构成的聚电解质溶液,模型的预测效果变差,有待进一步改进.该模型对两性聚电解质溶液渗透系数的预测效果比对聚电解质溶液的预测效果更好.     

Polyion interchange reactions of interpolyelectrolyte complexes in aqueous solutions and gels

Cooperative coupling reaction between two opposite charged polyelectrolytes results in formation of polyelectrolyte complexes (IPEC). This reaction is very fast and diffusion controlled. Whether IPECs formed by linear polyions are soluble or limitary swellable in aqueous media is decided by their composition, namely, by a ratio of oppositely charged polyions as well as by a water phase composition (the nature and the concentration of a simple salt, pH, the presence and the concentration of organic additives etc.). The most important intrinsic property of IPECs is their ability to participate in interchange (exchange and substitution) reactions with competing polyions. The kinetics and the position of equilibria in these reactions are controlled by the low molecular salt concentration, the nature of small counterions, DP of interaction polyelectrolytes, as well as by their linear charge density. IPECs can be formed also by interacting linear and opposite charged networks. It is shown that linear polyelectrolytes dissolved in aqueous solution can penetrate unexpectedly fast into oppositely charged cross-linked polyelectrolyte gels to form “snake-in-cage” composites representing IPECs of corresponding polyion segments. It is proved that the mechanism consists in “relay-race” transfer of linear polyion segments from one segment of the polyelectrolyte network to the other via interpolyelectrolyte exchange reaction. The driving force for the fast transport of linear polyions into the gel is produced by coupling reaction between two polyelectrolytes proceeding on solution/gel interface.     

Dielectric scaling in polyelectrolyte solutions with different solvent quality in the dilute concentration regime

In this note, we present a set of radiowave dielectric spectroscopy measurements of two dilute, differently-charged polyelectrolyte solutions, under different solvent conditions. We have found that both the dielectric strength, Delta epsilon, and the relaxation time, tau(ion), of the dielectric relaxation process associated with the counterion polarization along a length scale of the order of the correlation length obey the scaling laws with the polyion concentration, according to the Ito model. This is verified with good accuracy independently of the quality of the solvent, which has been varied from poor to good solvent conditions. This finding supports evidence to the fact that, in dilute solutions, the counterion polarization is independent of the polyion concentration, in spite of what occurs at the semi-dilute concentrations.     

End effects for a rodlike polyelectrolyte molecule in salt solution

Electrostatic potentials around a single rodlike polyelectrolyte molecule are calculated by solving the nonlinear Poisson–Boltzmann equation numerically in the presence of externally added salt. The polyion is regarded as a cylinder with a finite length whose side surface is uniformly charged and end surfaces uncharged. The calculations show that the distance to which end effects extend is about half the Debye screening length and is almost independent of the surface charge density and concentration of added salt. For a long polyion whose length is much greater than the Debye length, the end effects can be neglected even for a polyelectrolyte with high surface charges, whereas they play an important role for a short polyion with a length of the same order as the Debye length. In addition, a strong charge condensation is found in the direction of the axis of the cylinder for a long polyion.     

Ionic correlations in the inhomogeneous atmosphere surrounding cylindrical polyions: catalytic effects of polyions

The structural properties of linear polyelectrolyte solutions in the presence of a salt as evidenced through ionic correlations in the inhomogeneous atmosphere around a polyion and their consequence such as the catalytic potential are studied by using Monte Carlo simulation techniques. The simulations are performed on the cylindrical cell model where a uniformly charged hard cylinder mimics the linear polyion, which is caged in its own cylindrical cell containing counterions and salt. The cell (volume) average of the interionic correlations is presented as a function of the polyion and salt concentrations and ion radius. These results are utilized to study the catalytic effects of polyions as manifested through the changes in the collision frequency between ions in the double layer surrounding the polyion relative to that in the pure electrolyte solution. The reported results suggest a strong influence of the added salt/polyelectrolyte concentration ratio on the structural properties of the solution and hence on ion-ion collision frequency. The machine simulations are supplemented by nonlinear Poisson-Boltzmann results. Fair agreement between two different theoretical methods of calculating the collision frequency is obtained.     

Counterion-counterion correlation in the double layer around cylindrical polyions: counterion size and valency effects

Monte Carlo simulation and Poisson-Boltzmann results on some aspects of structure and thermodynamics of aqueous polyelectrolyte solutions are presented. The polyelectrolyte solution is described by an infinitely long cylindrical polyion surrounded by counterions modeled as rigid ions moving in a continuum dielectric. Ion-ion correlations in the form of volume average of the counterion-counterion distribution function in the double layer surrounding the polyion are reported for mono- and divalent counterions and for a range of polyion concentrations and charge density parameters in each case. These results confirm again strong influence of the charge density parameter of polyions on properties of polyelectrolyte solutions. The structural information is supplemented by the calculated thermodynamic properties such as osmotic coefficients and heats of dilutions; the latter quantity has not been examined yet in detail by computer simulations. The results are discussed in view of the existing experimental data from the literature for these properties.     

Neutron scattering from polyelectrolyte solutions

The neutron scattering intensity from polyelectrolyte solutions is calculated using an asymmetric primitive model electrolyte for the computation of the partial structure factors and a Debye function for the polyion form factor. The variation of the intensity with wavevector and concentration agrees with experimental results.