离子效应对纳滤膜表面Zeta电位测定的影响

采用流动电位法,用固体表面电位测定仪考察电解质溶液种类、浓度、p H对纳滤膜表面Zeta电位的影响。结果表明,二价离子溶液比一价离子溶液对纳滤膜表面Zeta电位作用明显,同价态离子的离子半径越小,Zeta电位越大;随着离子强度的增加,Zeta电位越小,在低离子浓度下Zeta电位值稳定性,重复性好;随着溶液p H的变化(3~10),纳滤膜的表面呈现两性性质,等电位点在p H 4.5~5.0之间。在测试纳滤膜表面Zeta电位时,推荐选择0.001mol/L的KCl电解质溶液。     

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.     

聚乙烯醇硫酸钾水凝胶电机械化学行为研究

通过将交联聚乙烯醇硫酸酯化的方法制备了一种新型电刺激响应性聚乙烯醇硫酸钾(PVSK)智能水凝胶,并探讨了溶液离子强度和pH对PVSK水凝胶的溶胀吸水率、机械性能以及电机械化学行为的影响.结果表明,制备的PVSK水凝胶的平衡溶胀比随NaCl溶液离子强度的增大而减小,在pH2.39～10.83范围内基本不受溶液pH的影响;经不同离子强度和pH的NaCl溶液充分溶胀的PVSK水凝胶具有良好的机械性能,在非接触的直流电场作用下,该水凝胶向电场负极弯曲,凝胶的弯曲速度和弯曲偏转量随外加电场强度的增加而增大,随NaCl溶液离子强度的增大出现临界最大值,但不随溶液pH(2.08～10.53)的改变而改变;在循环电场作用下,PVSK水凝胶的电机械化学行为具有良好的可逆性.     

聚乙烯醇磷酸酯水凝胶电刺激响应行为的研究

以脲为催化剂,将聚乙烯醇(PVA)磷酸酯化制成聚乙烯醇磷酸酯,再经戊二醛交联制备了一种新型的聚乙烯醇磷酸酯水凝胶.研究了水凝胶的溶胀性能,力学性能和电刺激响应行为.结果表明,该凝胶在NaCl水溶液中其平衡溶胀率随NaCl溶液的离子强度增大而减小.在离子强度为0~0.2的NaCl水溶液中,其弹性模量为0.300~0.356 MPa,抗张强度为91.5~137.8 kPa,断裂伸长率为32.0%~37.5%,且均随离子强度的增大而增大.在去离子水和NaCl水溶液中于非接触直流电场作用下,凝胶向电场负极弯曲,弯曲速度和应变随外加电压的增大而增大,并随NaCl离子强度的增大于0.005处出现极大值.在循环电场作用下,聚乙烯醇磷酸酯水凝胶的电刺激响应行为具有良好的可逆性.     

酯化淀粉乳化剂制备的高效氯氟氰菊酯O/W乳液的稳定机制

通过测定辛烯基琥珀酸淀粉钠的用量、盐离子、pH值和温度等因素对油滴Zeta电位及表面吸附量的影响,分析了以酯化淀粉辛烯基琥珀酸淀粉钠为乳化剂制备的5％高效氯氟氰菊酯水乳剂的稳定机制.结果表明,辛烯基琥珀酸淀粉钠质量分数为7％时,Zeta电位达到最大值,油滴表面吸附量接近饱和;Na+、Mg2+和Al3+压缩油滴表面的双电层,降低Zeta电位,削弱静电排斥作用,增加辛烯基琥珀酸淀粉钠分子柔性,提高辛烯基琥珀酸淀粉钠表面吸附量,且随着Na+、Mg2、Al3+离子强度依次增大,压缩双电层能力依次增强,Zeta 电位降低和表面吸附量增加程度依次增大;pH值影响辛烯基琥珀酸淀粉钠在水中的解离,在碱性范围内解离出较多羧酸根,静电排斥力较大,Zeta电位较高,但表面吸附量有所降低;温度升高,辛烯基琥珀酸淀粉钠在水溶液中溶解度增大,呈舒展状态,且辛烯基琥珀酸淀粉钠从油滴表面逃逸的趋势增加,油滴表面Zeta电位和表面吸附量均随着温度升高而降低,在低温区差别不大,温度越高二者变化越明显.辛烯基琥珀酸淀粉钠通过吸附于油滴表面为其提供较强的静电斥力和空间位阻作用而维持O/W乳液稳定.     

Zeta电位和界面膜强度对水包油乳状液稳定性影响

通过对表面活性剂、聚合物溶液和煤油体系油水界面剪切黏度和油珠的Zeta电位的测定,考察了界面膜强度和Zeta电位对水包油乳状液稳定性的影响。在煤油、表面活性剂、聚合物聚丙烯酰胺(3530S)或其氧化降解聚合物体系中,含有3530S时,界面膜强度值最大,最大值大于0.10 mN/m,Zeta电位为-18.4 mV,绝对值最大,乳状液最稳定。结果表明,油水界面膜强度和油珠表面的Zeta电位对水包油乳状液稳定性影响较大。界面膜强度和Zeta电位绝对值较大时,乳状液最稳定;当界面膜强度相差不大时,Zeta电位绝对值大的乳状液较稳定,此时双电层对乳状液稳定性起主要作用;当Zeta电位相差不大时,界面膜强度大的乳状液较稳定,此时界面膜强度对乳状液稳定性起主要作用。研究还表明,机械或氧化降解后的聚合物体系,界面剪切黏度和Zeta电位绝对值变小,乳状液稳定性变差。     

明胶水凝胶电刺激响应行为的研究

制备了戊二醛交联的明胶水凝胶 ,并研究了其吸水率、力学性能和电刺激响应行为 .结果表明 ,在NaCl溶液中 ,明胶水凝胶的平衡溶胀比随NaCl溶液的浓度增大而减小 ,经 0 0 1mol LNaCl溶液充分溶胀的明胶水凝胶膜其弹性模量为 4.2 9kPa ,抗张强度为 5 11kPa ,断裂伸长率为 110 %.在NaCl溶液中于非接触的直流电场作用下 ,明胶水凝胶向电场负极弯曲 ,凝胶的弯曲速度和弯曲偏转程度随外加电场的增大而增大 ,随NaCl溶液离子强度的增大出现临界最大值 .在周期性电场作用下 ,其弯曲响应行为具有良好的可逆性 .通过聚电解质凝胶弯曲理论初步解释了其弯曲机理 .     

温度、pH敏感性核壳结构微凝胶的制备及性质

以无皂乳液分步聚合的方法, 将N-异丙基丙烯酰胺(NIPAM)与N,N-亚甲基双丙烯酰胺(MBA)交联反应3 h, 制得种子乳液, 再向种子乳液中加入甲基丙烯酸(MAA)功能性单体继续反应2 h, 制备了具有温度、pH敏感性的核壳结构微凝胶. 通过透射电子显微镜(TEM)、红外光谱(IR)等表征了微凝胶外貌形态及结构组成, 动态光散射(DLS)测定了微凝胶粒径响应热、pH的变化及微凝胶Zeta电位的变化. 结果表明凝胶形貌为异型核壳结构; Zeta电位与微凝胶粒径随温度、pH变化相关.     

从银电极上氢析出的温度效应得到的反应动力学启示

利用循环伏安法研究了多晶银电极在0.1 mol/L HClO4溶液中氢析出反应的温度效应. 发现当从析氢起始电位负向扫描至零电荷电位（-0.4 V）时,氢析出反应的表观活化能（Ea,app）和指前因子（A）均随着电势的负移而增大（对应的Ea,app从24 kJ/mol增大至32 kJ/mol）.继续负向扫描至零电荷电位以后,Ea,app随电势的负移而减小但A不随电势变化. 推测Ea,app和A在零电荷电位前的反常变化来自于反应物和过渡态之间内能和熵值变化．在零电荷电位以正电位,电极附近的水分子以氧端吸附在电极表面上,且水分子之间有氢键作用。电势变化产生的能量主要用于使水分子脱附并使氢键网络改变．在E〉PZC的电位区,电位负移导致的正的熵效应（指前因子增加）补偿了活化能的升高导致的负效应,从而显示反应的净电流随电位负移而增加．结果表明溶剂的动力学和相关的熵因子项可能会对析氢这类涉及质子和电子转移的电极反应的动力学产生很大的影响．     

离子键交联的聚两性电解质凝胶在不同pH和不同电解质溶液中溶胀行为研究

以丙烯酸(AA)和甲基丙烯酸二乙氨基乙酯(DEAM)形成的离子复合物与丙烯酰胺(AAm)共聚,合成了一种新型的离子键交联的聚两性电解质凝胶(PADA).由于分子之间的氢键作用,PADA凝胶并不是在A/C(负正离子单体摩尔比)为1,而是在A/C为1.55处有最大消溶胀.与共价键交联的聚两性电解质凝胶相比,PADA凝胶的溶胀行为具有更强的pH敏感性.PADA凝胶在不同pH缓冲溶液中的溶胀行为表明,在pH 3~4之间消溶胀程度最大.在偏离该pH区域时凝胶均发生溶胀.但凝胶的溶胀程度在pH<3的酸性溶液中随A/C的增加而降低;而在pH>4的偏碱性溶液中随其增加而增加.在不同价数的离子溶液中,离子浓度对于PADA凝胶的平衡溶胀有着不同的影响.对于一价的NaCl溶液,PADA凝胶有典型的反聚电解质效应.但对于高价的CaCl2和柠檬酸三钠溶液,只在较低的浓度下,才表现出反聚电解质效应.而在较高盐浓度时,随盐浓度的增加其溶胀比反而降低.这可能与高价离子形成的离子键交联有关.与pH对PADA凝胶溶胀程度的影响相似,在CaCl2溶液中,PADA凝胶的溶胀程度随A/C的增加而降低;而在柠檬酸三钠溶液中则刚好相反.这种独特的溶胀行为似乎与高价离子电荷的正负性有关.     

Flocculation of microgel particles with sodium chloride and sodium polystyrene sulfonate as a function of temperature

The flocculation behavior of poly(N-isopropylacrylamide) (PNIPAM) microgel particles, containing surface sulfate groups, has been studied as a function of sodium chloride [NaCl] concentration, between 0.1 and 800 mM NaCl and over the temperature range 25-60 degrees C. The critical flocculation temperature (CFT) of the particles was determined as a function of NaCl concentration. Three regions of NaCl concentration were established. First, at very low values of [NaCl] (< approximately 25 mM), no CFT value could be determined; this implies that the interparticle electrostatic repulsion is sufficient to prevent any flocculation occurring. This remains the case even at temperatures well in excess of the lower critical solution temperature for PNIPAM in solution, where the particles are essentially deswollen. Second, at intermediate [NaCl] (approximately 25-100 mM), the CFT decreased strongly with increasing [NaCl]. In this region, the electostatic forces are weakened sufficiently for the van der Waals forces to cause flocculation. Third, at higher [NaCl] (> approximately 100 mM), the electrostatic repulsion is screened out, and the CFT decreases linearly with [NaCl]. The reason for this decrease is the fact that aqueous solutions of NaCl become increasingly poorer solvent environments for PNIPAM with increasing [NaCl]. These trends are apparent also in the values determined for the hydrodynamic size of the stable PNIPAM particles as a function of [NaCl] and temperature. It is shown that the flocculation of the PNIPAM particles is consistent with a weak, reversible flocculation model. This is apparent, for example, from the fractal dimensions of the flocs (approximately 2.0), determined from the power law used to fit the time evolution of the hydrodynamic size of the flocs, and also from the estimated depth of the mimimum in the interparticle pair potential, based on the critical size of the primary particles where flocculation just begins to occur. The effect of adding sodium poly(styrene sulfonate) [PSS] to the PNIPAM dispersions, in the absence of NaCl, was also investigated. The minimum amount of PSS required to induce flocculation was found to decrease with increasing temperature.     

K2FeO4-Zn碱性固态电解质电池电化学性能研究

应用溶液铸膜法制备出了交联聚乙烯醇(PVA)/聚丙烯酸(PAA)-KOH-H2O复合碱性固态电解质膜, 其厚度为150 µm左右, SEM测试结果表明其表面呈均相的非晶态结构, 交流阻抗(EIS)测试表明室温离子电导率可达3.5×10－2 S&#8226; cm－1, 循环伏安(CV)测试表明其电化学稳定窗口为3.5 V左右, 将其应用于一次碱性K2FeO4-Zn电池, 通过研究固态电解质膜在不同浓度KOH碱液中预处理和其在不同放电倍率下的放电性能, 结果表明, 9 mol&#8226;L－1为最佳固态电解质膜预处理碱液浓度, 0.4 C为最佳放电倍率, 1.0 V以上容量最高可达222.6 mAh&#8226;g－1, 并表现出良好的放电平台特性.     

La 0.9 M 0.1 Ga 0.8 Mg 0.2 O 3 -α的中温质子导电性及其在常压合成氨中的应用

采用水热沉淀法制备了La0.9M0.1Ga0.8Mg0.2O3-α (M＝Ca2＋, Sr2＋, Ba2＋)陶瓷样品的前驱体, 沉淀剂来自尿素在水热条件下的水解产物. 前驱体经煅烧和烧结后得到陶瓷样品. XRD显示样品具有单一的斜方晶LaGaO3钙钛矿结构. 同位素效应和氢的电化学透过(氢泵)实验证明陶瓷样品具有质子导电性. 用AC阻抗谱法测定了样品在300～600 ℃、氢气气氛中的质子电导率, 其大小取决于La位掺杂的碱土金属离子: σ(M＝Sr2＋)＞σ(M＝Ba2＋)＞σ(M＝Ca2＋). 以La0.9M0.1Ga0.8Mg0.2O3-α为固体电解质进行了常压合成氨, 最佳合成温度为520 ℃. 当施加的电流密度为1 mA&#8226;cm－2、合成温度为520 ℃时, 氨产率分别为: 1.63×10–9 mol&#8226;s－1&#8226;cm－2 (M＝Ca2＋), 2.53×10－9 mol&#8226;s－1&#8226;cm－2 (M＝Sr2＋)和2.04× 10－9 mol&#8226;s－1&#8226;cm－2 (M＝Ba2＋).     

铁氰化镧修饰电极的制备及表征

An electroactive polynuclear inorganic compound of rare earth metal hexacyanoferrate, lanthanum hexacyanoferrate (LaHCF), was prepared by electrochemical deposition on the surface of a glassy carbon electrode with a potential cycling procedure. The cyclic voltammogram of LaHCF exhibits a pair of well-defined redox peaks with the formal potential of 208 mV (vs. SCE) at a scan rate of 100 mV/s in 0.2 mol/L NaCl solution and the redox peak currents increase linearly with the square root of the scan rate up to 1000 mV/s. The effects of the concentration of supporting electrolyte on the electrochemical characteristics of LaHCF were studied by voltammetry. LaHCF was also characterizated by scanning electron microscope (SEM), FTIR and XPS techniques.     

Polymerized rodlike nanoparticles with controlled surface charge density

Stable rodlike nanoparticles with highly controlled surface charge density have been developed by the free radical polymerization of the mixture of polymerizable cationic surfactant, cetyltrimethylammonium 4-vinylbenzoate (CTVB), and hydrotropic salt sodium 4-styrenesulfonate (NaSS) in aqueous solution. The surface charge of the polymerized CTVB/NaSS rodlike nanoparticles was controlled by varying the NaSS concentration during the polymerization process, and the charge variation was interpreted in terms of the overcharging effect in colloidal systems. The SANS measurements show that the diameter of the polymerized CTVB/NaSS rodlike nanoparticles is constant at 4 nm and the particle length ranges from 24 to 85 nm, depending on the NaSS concentration. The polymerized particles are longest when the NaSS concentration is 5 mol % which corresponds to the charge inversion or neutral point. The SANS and zeta potential measurements show that the Coulomb interactions between the particles are strongly dependent on the NaSS concentration and the zeta potential of the polymerized CTVB/NaSS nanoparticles changes from positive to negative (+12.8 approximately -44.2 mV) as the concentration of NaSS increases from 0 to 40 mol %. As the NaSS concentration is further increased, the zeta potential is saturated at approximately -50 mV.     

Fibrinogen adsorption on mica studied by AFM and in situ streaming potential measurements

Adsorption of fibrinogen from aqueous solutions on mica was studied using AFM and in situ streaming potential measurements. In the first stage, bulk physicochemical properties of fibrinogen and the mica substrate were characterized for various ionic strength and pH. The zeta potential and number of uncompensated (electrokinetic) charges on the protein surfaces were determined from microelectrophoretic measurements. Analogously, using streaming potential measurements, the electrokinetic charge density of mica was determined for pH range 3-10 and the NaCl background electrolyte concentration of 10(-3) and 10(-2) M. Next, the kinetics of fibrinogen adsorption at pH 3.5 and 7.4 in the diffusion cell was studied using a direct AFM determination of the number of molecules per unit area of the mica substrate. Then, streaming potential measurements were performed to determine the apparent zeta potential of fibrinogen-covered mica for different pH and ionic strength in terms of its surface concentration. A quantitative interpretation of these streaming potential measurements was achieved in terms of the theoretical model postulating a side-on adsorption of fibrinogen molecules as discrete particles. On the basis of these results, the maximum coverage of fibrinogen Θ close to 0.29 was predicted, in accordance with previous theoretical predictions. It was also suggested that anomalous adsorption for pH 7.4, where fibrinogen and the mica substrate were both negatively charged, can be explained in terms of a heterogeneous charge distribution on fibrinogen molecules. It was estimated that the positive charge was 12 e (for NaCl concentration of 10(-2) M and pH 7.4) compared with the net charge of fibrinogen at this pH, equal to -21 e. Results obtained in this work proved that the coverage of fibrinogen can be quantitatively determined using the streaming potential method, especially for Θ < 0.2, where other experimental methods become less accurate.     

Temperature Effect on Hydrogen Evolution Reaction at Au Electrode

The temperature dependence of hydrogen evolution reaction (HER) at a quasi-single crys-talline gold electrode in both 0.1 mol/L HClO₄ and 0.1 mol/L KOH solutions was investigated by cyclic voltammetry. HER current displays a clear increase with reaction overpotential (η) and temperature from 278～333 K. In 0.1 mol/L HClO₄ the Tafel slopes are found to increases slightly with temperature from 118 mV/dec to 146 mV/dec, while in 0.1 mol/L KOH it is ca. 153±15 mV/dec without clear temperature-dependent trend. The apparent activation energy (Ea) for HER at equilibrium potential is ca. 48 and 34 kJ/mol in 0.1 mol/L HClO₄ and 0.1 mol/L KOH, respectively. In acid solution, Ea decreases with increase in η, from Ea=37 kJ/mol (η=0.2 V) to 30 kJ/mol (η=0.35 V). In contrast, in 0.1 mol/L KOH, Ea does not show obvious change with η. The pre-exponential factor (A) in 0.1 mol/L HClO₄ is ca. 1 order higher than that in 0.1 mol/L KOH. Toward more negative potential, in 0.1 mol/L HClO₄ A changes little with potential, while in 0.1 mol/L KOH it displays a monotonic increase with η. The change trends of the potential-dependent kinetic parameters for HER at Au electrode in 0.1 mol/L HClO₄ and that in 0.1 mol/L KOH are discussed.     

酶法拆分(±)-N-(2,6-二甲苯基)-丙氨酸甲酯

用脂肪酶Candida rugosa lipase (CRL)拆分(±)-N-(2,6-二甲苯基)-丙氨酸甲酯, 并进一步优化反应条件. 结果表明, 在加入1 mmol N-(2,6-二甲苯基)-丙氨酸甲酯、100 mL的0.2 mol/L磷酸缓冲液中, CRL拆分该底物的最适反应条件为: pH 6.4, CRL脂酶250 mg, 聚乙二醇(PEG) 2 g, 转速160 r•min^－1, 温度 35 ℃. 其中酶量、温度对转化率影响较大. 反应后分离得R-(＋)-N-(2,6-二甲苯基)-丙氨酸甲酯. 它和酰氯反应可制备一系列旋光性N-酰基丙氨酸类杀菌剂.     

室温离子液体增塑的纳米复合聚合物电解质研究

在室温离子液体N-乙基-N'-甲基咪唑四氟硼酸盐(EMIBF₄)增塑的凝胶聚合物电解质中加入氧化铝纳米粒子, 制备了一种纳米复合聚合物电解质(nanocomposite polymer electrolyte, NCPE). 通过示差扫描量热(DSC)、X射线衍射(XRD)、热重分析(TGA)、电化学阻抗谱(EIS)等手段对其进行了表征. 结果显示, 随着氧化铝纳米粒子含量的增加, NCPE的结晶度降低, 离子导电率升高. 但是, 纳米粒子的加入量过大时反而引起NCPE的离子导电率降低. 当纳米粒子填充量为w＝10%时, NCPE具有最高的室温离子导电率1.25×10^－3 S•cm^－1.     

新型氧离子导体La2Mo1.8Ga0.2O9陶瓷的合成及其电性能

通过高温固相合成法首次合成了La₂Mo_1.8Ga_0.2O₉陶瓷样品. 粉末XRD结果表明, 该样品为单一立方相La₂Mo₂O₉结构. 以陶瓷样品为固体电解质、多孔性铂为电极, 采用交流阻抗谱、气体浓差电池、氧泵等方法研究了样品在600～1000 ℃下各种气氛中的离子导电特性. 结果表明, 氧浓差电池电动势的实测值与理论值吻合得很好, 氧离子迁移数为1, 表明该陶瓷样品在该温度下氧气气氛中为一纯氧离子导体; 氧泵(氧的电化学透过)实验结果进一步证实了该样品在氧气气氛中为一纯氧离子导体; 在氧分压p(O₂)＝10^－5～10⁵ Pa的高氧分压气氛中, 电导率与氧分压变化基本无关, 表明在该氧分压范围内样品为纯离子导体, 这与氧浓差电池电动势测定结果相吻合; 在低氧分压为10^－5～10^－15 Pa范围内, 总电导率随氧分压降低而稍有升高, 表明在该氧分压范围样品为氧离子与电子的混合导体; 在600～1000 ℃下氧离子电导率＞10^－2 S•cm^－1, 显著高于母体La₂Mo₂O₉的氧离子电导率, 1000 ℃时的氧离子电导率为0.07 S•cm^－1.