电解质对带电磷脂自组装行为的影响

运用光学显微镜研究了电解质对心磷脂聚集形态的影响. 结果表明, 阳离子的价态和浓度对心磷脂的聚集形态有很大影响, 而离子半径及同一价态下离子种类的影响相对较小. 在一定浓度范围的一价电解质溶液中, 可见同中心的多层管状囊泡的生长, 而且囊管的长度L与生长时间t的标度关系不因电解质种类和浓度的改变而改变. 随着电解质浓度的增加, 除通常的囊管结构外, 还出现了单螺旋、双螺旋甚至超螺旋的结构.     

钙离子和镁离子浓度变化对磷脂酰乙醇胺-磷脂酰甘油双分子层膜的影响

Ca²⁺ and Mg²⁺ ions are the main divalent cations in living cells and play vital roles in the structure and function of biological membranes. To date, the differences in the effects of these two ions on the Escherichia coli (E. coli) inner membrane at various concentrations remain unknown. Here, the effects of Ca²⁺ and Mg²⁺ ions on a mixed lipid bilayer composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoethanolamine (POPE) and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG) in a 3 : 1 ratio (mol/mol), which mimics the E. coli inner membrane, were quantitatively differentiated at different concentrations by dynamic light scattering (DLS), zeta potential measurements and all-atom molecular dynamics (AA-MD) simulations. The DLS results demonstrated that the POPE/POPG liposomes were homogeneous and monodisperse in solutions with Ca²⁺ or Mg²⁺ ion concentrations of 0 and 1 mmol∙L^-1. As the Ca²⁺ or Mg²⁺ ion concentration was increased to 5-100 mmol∙L^-1, lipid aggregation or the fusion of unilamellar liposomes occurred in the ion solutions. The zeta potential measurements showed that both the Ca²⁺ and Mg²⁺ ions had overcharging effects on the negatively charged POPE/POPG liposomes. The AA-MD simulation results indicated that the Ca²⁺ ions irreversibly adsorbed on the membranes when the simulation time was longer than 100 ns, while the Mg²⁺ ions were observed to dynamically adsorb on and desorb from the membranes at various concentrations. These results are consistent with the DLS and zeta potential experiments. The average numbers of Ca²⁺ and Mg²⁺ ions in the first coordination shell of the oxygen atoms of the phosphate, carbonyl and hydroxyl groups of POPE and POPG (i.e., the first coordination numbers) in the pure membrane and membranes containing 5 and 100 mmol∙L^-1 ions were calculated from the radial distribution functions. The results indicated that the primary binding site of these two ions on POPE and POPG at the concentrations studied was the negatively charged phosphate group. Thus, these results might explain the overcharging effects of both the Ca²⁺ and Mg²⁺ ions on the POPE/POPG liposomes. Moreover, as the Ca²⁺ concentration increased, the area per lipid of the lipid bilayers decreased, and the membrane thickness increased, while the Mg²⁺ ions had negligible effects on these membrane parameters. In addition, these ions had different effects on the orientation of the lipid head groups. These simulation results may be used to provide the possible explanations for the differences between Ca²⁺ and Mg²⁺ ions in DLS and zeta potential measurements at the atomic level. The experimental results and MD simulations provide insight into various biological processes regulated by divalent cations, such as membrane fusion.     

铂电极B-Z反应系双电层稀疏区电势跃变对电化学振荡的影响

根据连续步骤间非平衡耗散的特征, 定量表示了电化学步骤与扩散步骤的相对滞后性对电极反应体系耗散的贡献, 建立了稀疏区电势跃变ψ的非平衡态热力学计算公式, 给出了其在Boltzman分布近似下的表现形式. 同时, 建立了一个普适的Pt电极B-Z反应动力学模型, 讨论了ψ对电极B-Z反应系状态演化动力学行为的影响, 发现ψ的引入将强化该电极反应体系动力学机制的非线性程度, 导致电化学振荡区的蜕变. 给出了相应的计算机模拟图谱.     

离子浓度对电纺纤维沉积形态及表面形貌的影响

通过采用传统电纺丝装置(接收板接地或连接负压电源)、逆向电场及非接触式电纺丝装置等4种不同的电纺丝装置,在相同电压、接收距离、纺针直径、温湿度条件下,对20%的聚乙烯醇溶液进行电纺丝实验,观察不同装置中制得的纤维的沉积形态与形貌.还采用ANSYS有限元模拟对电纺丝装置的场强分布进行分析,并引入电化学理论解释了采用不同电纺装置时离子浓度的不同对所得电纺纤维形貌的影响,分析了产生差异的原因.     

聚电解质结构及盐浓度对基于DNA和聚阳离子的层层组装型大孔薄膜结构的影响

选择2种不同类型的聚阳离子[强电解质型聚二烯丙基二甲基氯化铵(PDDA)和弱电解质型聚盐酸丙烯胺(PAH)], 分别和脱氧核糖核酸(DNA)分子通过静电吸附作用制备层层组装膜. 利用原子力显微镜和紫外-可见分光光度计研究了聚阳离子结构和组装分子溶液中盐(NaCl)浓度对大孔结构及薄膜生长规律的影响. 结果表明, 在DNA/PDDA体系中, 盐浓度对于大孔结构的形成起到关键性作用. 而对于DNA/PAH薄膜体系, 即使增加DNA或PAH溶液中盐的浓度, 也不会有大孔结构出现, 这主要是由PAH分子的弱电解质特性决定的.     

PS-PBA粒子分散系的介电弛豫谱解析——同、反离子对弛豫的影响及表界面电参数的计算

制备了近纳米级的聚苯乙烯-丙烯酸丁酯(PS-PBA)复合微球粒子,并在40Hz～110×106Hz的宽频范围测量了该粒子分散在9种电解质中时的介电弛豫谱,发现了与PS微球粒子分散系不同的特异介电弛豫:低频弛豫对反离子种类具有敏感性而高频弛豫则与电解质种类几乎无关;根据Shilov-Dukhin模型和M-W-O模型分别分析了高、低频率的弛豫机制,并通过对介电谱的Cole-Cole拟合获得了各体系的介电参数.进一步利用Hanai方法由介电参数计算获得了所有体系的相参数;详细分析了体系的内部参数受PS-PBA微球自身结构以及电解质种类影响的原因;讨论了离子扩散系数对介电参数的影响,从而得出了低、高频的弛豫特征时间分别由同离子的扩散系数和反离子的扩散系数所决定之结论.最后,结合Grosse宽频介电理论计算了粒子表面的以及双电层的主要电参数,并分析了电解质种类差异对这些电参数的影响.     

表面活性剂对硫醇单层膜修饰金电极电化学行为的影响

利用自组装方法在金电极表面制备成硫醇单层膜, 循环伏安和交流阻抗实验表明硫醇单层膜与表面活性剂十六烷基三甲基溴化胺作用后, 其电化学行为发生变化, 对于带有不同电荷的探针分子, 表现出一定的选择性响应. 即使是带有相同电荷的探针分子, 由于与表面活性剂的作用方式不同, 也使它们通过硫醇单层膜在电极表面产生电化学响应的程度完全不同.     

前驱体分子结构对聚糠醇基碳膜微结构及气体分离性能的影响

分别以草酸(OA)和碘(I)两种催化剂合成聚糠醇(PFA)前驱体制备气体分离碳膜. 采用TG, FTIR和XRD对其微结构进行研究, 并通过纯组分气体的渗透实验对碳膜的分离性能进行了探讨. 研究结果表明, 在热解过程中, 两种结构的聚糠醇都是通过脱氧、重排、环化、芳构化等热分解和热缩聚反应逐渐转化为无定形的乱层碳结构, 但热分解反应过程明显不同, 所形成碳膜微结构的差异也很大. 草酸催化剂制备的聚糠醇碳膜的微晶Lc值比碘催化剂制备碳膜的大, 而d(002)和La值则比后者的小, 表明草酸催化剂制备的聚糠醇碳膜碳微晶片层数多、排列规则、结构缺陷和孔隙均小于碘催化剂制备的聚糠醇碳膜, 而且其气体分离选择性较高、渗透通量较小, 表明聚糠醇的分子结构对所制备碳膜的微结构及气体分离性能有很大影响.     

草酸钾诱导的LB膜缺陷及对草酸钙堆积图形的影响

采用扫描电子显微镜(SEM)和原子力显微镜(AFM)研究了经不同浓度草酸钾(K2C2O4)处理后二棕榈酰磷酯酰胆碱(DPPC)的缺陷LB膜及其对一水草酸钙(COM)成核和生长的影响. K2C2O4的处理可进一步破坏LB膜中圆形畴区内的分子列阵, 尤其是使处在液态扩张相(LE)/液态凝集相(LC)边界的分子列阵无序程度增加, 从而促进了COM晶体在此处的成核和生长, 最终诱导圆形堆积的COM晶体图形出现. 随着损伤LB膜的K2C2O4浓度c(K2C2O4)从0.3 mmol/L增加到5.0 mmol/L, 其对LB膜畴区有序结构的破坏作用逐渐增强, 圈状堆积的晶体图形数量增多. 当c(K2C2O4)为0.3 mmol/L时, 主要诱导实心的圆形堆积的COM晶体图形, 而当c(K2C2O4)增加至5.0 mmol/L时, 生成圈状COM晶体图形, 且图形的半径减小. 这一研究结果将有助于从分子和超分子水平上了解肾小管上皮细胞膜损伤后的微结构变化及其与肾结石形成的关系.     

钯/聚苯胺纳米多层膜的制备及对抗坏血酸和多巴胺的催化氧化

采用脉冲电位法(PPSM)结合聚苯胺(PANI)的层层自组装制备了Pd/PANI交替沉积纳米多层膜, 并用于抗坏血酸(AA)和多巴胺(DA)的检测. 实验发现, 多层膜结构形貌及催化性能受前躯体K₂PdCl₆浓度、 脉冲条件及膜厚度等影响. 当K₂PdCl₆浓度为2×10^-3 mol/L, 阴极脉冲电位为-0.3 V, 阶跃次数为17时, 5层Pd/PANI修饰玻碳电极对AA和DA的催化性能最佳; 在0.1 mol/L磷酸盐缓冲液中, AA和DA的氧化峰明显分离[ΔE_p(AA, DA)=160 mV], 其峰电流与浓度分别在5×10^-5～4×10^-4和4×10^-5～1×10^-4 mol/L范围内呈较好线性关系, 实现了对AA和DA的同时测定. 该修饰电极具有良好的抗干扰性和稳定性.     

Effect of Electrolyte Concentration on the Stern Layer Thickness at a Charged Interface

The chemistry and physics of charged interfaces is regulated by the structure of the electrical double layer (EDL). Herein we quantify the average thickness of the Stern layer at the silica (SiO₂) nanoparticle/aqueous electrolyte interface as a function of NaCl concentration following direct measurement of the nanoparticles’ surface potential by X‐ray photoelectron spectroscopy (XPS). We find the Stern layer compresses (becomes thinner) as the electrolyte concentration is increased. This finding provides a simple and intuitive picture of the EDL that explains the concurrent increase in surface charge density, but decrease in surface and zeta potentials, as the electrolyte concentration is increased.     

细胞色素C在阴离子修饰的盐桥支撑双层类脂膜上的电化学行为及其应用

采用循环伏安法研究了细胞色素C在月桂酸阴离子修饰的盐桥支撑双层类脂膜上的氧化还原反应;对盐桥支撑双层类脂膜的特性、细胞色素C的电化学反应动力学以及有关影响细胞色素C循环伏安行为各种因素进行了详细探讨;并对用该双层类脂膜体系电化学测定细胞色素C进行了初步尝试。     

非支撑磷脂双层膜制备及温度对其力学性质的影响

结合聚苯乙烯球刻蚀和微机电系统技术加工氮化硅纳米多孔膜, 并在其上用囊泡法制备非支撑磷脂双层膜, 通过温控原子力显微术(AFM)的成像模式和力曲线模式对非支撑磷脂双层膜的形貌和力学性质进行研究. 实验结果表明, 该方法制备的非支撑磷脂双层膜具有流动性, 能进行自我修复, 该特点有利于提供足够的非支撑磷脂双层膜区域用于其性质研究; 非支撑磷脂双层膜的膜破力和粘滞力均随着温度的升高而减小, 即膜的机械稳定性随着温度的升高而降低. 非支撑磷脂双层膜膜破力小于支撑磷脂双层膜的膜破力, 并且非支撑磷脂双层膜粘滞力随温度的变化趋势与支撑磷脂双层膜的变化趋势相反.     

Similarities and Differences between Crystal and Enzyme Environmental Effects on the Electron Density of Drug Molecules

The crystal interaction density is generally assumed to be a suitable measure of the polarization of a low-molecular weight ligand inside an enzyme, but this approximation has seldomly been tested and has never been quantified before. In this study, we compare the crystal interaction density and the interaction electrostatic potential for a model compound of loxistatin acid (E64c) with those inside cathepsin B, in solution, and in vacuum. We apply QM/MM calculations and experimental quantum crystallography to show that the crystal interaction density is indeed very similar to the enzyme interaction density. Less than 0.1 e are shifted between these two environments in total. However, this difference has non-negligible consequences for derived properties.     

干相转换条件对致密皮层不对称膜结构及透气性能的影响

研究了挥发时间、温度等干相转换条件对聚芳醚砜致密皮层不对称膜形态结构、有效皮层厚度及氮、氢透过性能的影响．表明采用本铸膜液体系，在２０℃左右，很短的挥发时间内即可制得较理想的气体分离膜。