凝胶网格沉淀法制备纳米氧化锌的正交实验研究

通过凝胶网格沉淀法制备了纳米氧化锌,并通过正交实验探讨了明胶用量、锌离子浓度、碳酸根离子浓度以及反应物配比等因素对其粒径的影响。实验确定了制备纳米氧化锌的优化工艺条件:明胶用量22%、锌离子浓度0.7mol/L、碳酸根浓度0.7mol/L、反应物配比1/1。采用XRD、IR、TG-DTA、TEM及激光粒度等测试手段对产物进行了表征。结果表明,在优化工艺条件下制得了粒径为40nm的氧化锌。     

绿色和黄色银胶的光化学制备及其共振散射光谱研究

研究了不同光源、光照时间、反应物浓度等对绿色银胶形成的影响,分别制备了绿色银胶和黄色银胶.透射电镜显示,它们的平均粒径分别为100nm和40nm.绿色银胶在393.9nm和713.3nm处有两个吸收峰;黄色银胶在419.3nm处有一较宽的吸收峰.它们的最强共振散射峰位于470nm处;绿色银胶在340nm和80nm还有两个小共振峰.     

纳米银负载的炭气凝胶制备及抗菌性能研究

以常压干燥法制备的酚醛有机气凝胶为原料,通过在硝酸银溶液中浸渍使银吸附或沉积在有机气凝胶上,在常压条件下干燥并炭化制得纳米银负载的炭气凝胶。利用扫描电镜(SEM)、透射电镜(TEM)、X-射线衍射(XRD),比表面积及孔径分析等方法研究了浸渍前后凝胶密度和结构的变化,以及制备条件对银负载炭气凝胶的载银量和凝胶结构的影响;研究了载银炭气凝胶对大肠埃氏杆菌(ATCC25922)和金黄色葡萄球菌(ATCC25923)的抗菌效果。结果表明,这类银负载炭气凝胶对大肠杆菌和金黄色葡萄球菌均有很强的杀灭能力,预期炭气凝胶在作为催化剂或吸附杀菌材料方面有良好的应用前景。     

凝胶过滤-原子吸收光谱法在研究照相明胶中的应用

照相明胶中的微量金属元素对卤化银乳剂的性能有多方面的影响,所以研究照相明胶中金属杂质的总量,以及它们的化学形态对改善乳剂质量和生产优质照相明胶具有重要意义。本文以明胶中钙的测定为例探讨了凝胶过滤─-火焰原子吸收法在研究照相明胶中金属形态的特点,并且提出了不经消化或水解而用火焰原子吸收法直接测定明胶中钙的方法。     

聚离子液负载金纳米粒子水凝胶的制备及阴离子响应性

通过咪唑基离子液单体与二乙烯苯的自由基聚合制备了聚离子液水凝胶,并通过一步还原得到了离子液水凝胶负载金纳米粒子的复合材料。用UV-Vis光谱和透射电子显微镜研究了金纳米粒子在离子液水凝胶内部的分散状态及阴离子响应性聚集。结果表明,由于空间位阻和静电作用,制得的金纳米粒子的表面等离子共振吸收峰为527 nm,在离子液水凝胶中呈均匀分散的球形(2～5 nm);在PF6-阴离子的作用下,形成了疏水性水凝胶,使凝胶收缩,凝胶内部的金纳米粒子发生聚集,其吸收峰红移到532 nm,初步证实了此水凝胶具有阴离子响应性。     

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 .     

明胶凝胶表面润湿性的研究

本工作利用测定几种参照液体在明胶凝胶上的接触角,定量地估算了明胶凝胶的表面自由能。加入表面活性剂,尤其是非离子表面活性剂,能增加明胶凝胶的表面自由能(主要是其极性分量)并大大改善明胶凝胶的表面润湿性。在表面上分子的吸附与定向和明胶凝胶中非极性网状结构形成的基础上,解释了上述实验结果。     

银纳米颗粒负载阶层多孔二氧化硅块体的制备及表征

以溶胶-凝胶伴随相分离法制备的阶层多孔二氧化硅作为载体,3-氨丙基三乙氧基硅烷(APTES)为改性剂,乙醇为还原剂,在阶层多孔二氧化硅固体骨架上进行银纳米颗粒均匀负载.利用扫描电镜(SEM)、透射电镜(TEM)、X射线衍射(XRD)、汞压、N2吸附/脱附、X射线光电子能谱(XPS)等测试技术对银纳米颗粒负载阶层多孔二氧化硅进行了表征,探讨了APTES表面改性、乙醇还原机理以及银纳米颗粒负载块体的孔结构特征变化规律.结果表明:APTES表面改性将氨基接枝于阶层骨架上,氨基与银离子形成银氨离子,银氨离子经乙醇还原后将平均粒径约16 nm的银纳米颗粒成功负载于二氧化硅的大孔及介孔内部;负载后的阶层多孔块体的大孔骨架未受到破坏,但其比表面积由418 m2·g-1下降到254m2·g-1,两次还原负载能提高银纳米颗粒的负载量.     

凝胶网格控制合成纳米ZnO及其光催化活性

以明胶为反应介质,采用凝胶网格控制合成法制备了单分散球形纳米ZnO光催化剂.利用TG-DTA、XRD、TEM、BET、UV-Vis、HPLC等测试手段对制备过程、样品的结构和性能进行了研究,探讨了明胶浓度、煅烧温度对产物粒径和光催化活性的影响.结果表明:利用凝胶网格控制合成法不仅能够控制纳米微粒的形状和大小,而且可防止沉淀物相互聚集和团聚.以染料罗丹明B溶液为目标降解物,1 h的降解率为99.9%,最佳光催化剂的合成条件:13%明胶浓度、350℃煅烧2 h.     

银纳米颗粒负载阶层多孔二氧化硅块体的制备及表征

以溶胶-凝胶伴随相分离法制备的阶层多孔二氧化硅作为载体,3-氨丙基三乙氧基硅烷（APTES）为改性剂,乙醇为还原剂,在阶层多孔二氧化硅固体骨架上进行银纳米颗粒均匀负载. 利用扫描电镜（SEM）、透射电镜（TEM）、X射线衍射（XRD）、汞压、N₂吸附/脱附、X射线光电子能谱（XPS）等测试技术对银纳米颗粒负载阶层多孔二氧化硅进行了表征,探讨了APTES表面改性、乙醇还原机理以及银纳米颗粒负载块体的孔结构特征变化规律. 结果表明：APTES表面改性将氨基接枝于阶层骨架上,氨基与银离子形成银氨离子,银氨离子经乙醇还原后将平均粒径约16 nm的银纳米颗粒成功负载于二氧化硅的大孔及介孔内部;负载后的阶层多孔块体的大孔骨架未受到破坏,但其比表面积由418 m²·g^-1下降到254 m²·g^-1,两次还原负载能提高银纳米颗粒的负载量.     

Monodisperse copper‐ and silver‐nanocolloids suitable for heat‐conductive fluids

Copper colloid was prepared via reductive stabilization. The suspension of the trioctylaluminum‐stabilized copper colloid was peptized using Korantin SH and cashew nut shell liquid (CNSL). Fluids with particle sizes <10 nm were obtained with Korantin and 7–15 nm in the case of CNSL. However, the copper colloid is air sensitive. A very straightforward one‐step method leads to air‐stable silver nanofluids. Thermal decomposition of silver lactate in the presence of Korantin SH and mineral oil as the medium gave a silver nanofluid. Silver particle formation and air stability were monitored using UV–VIS spectroscopy. The presence of monodispersed spherical silver nanoparticles was confirmed. Transmission electron microscopy showed a two‐dimensional assembly of the silver particles with a size distribution of 9.5 ± 0.7 nm. FTIR has revealed information about the interaction between the surfactant and the silver surface. Copyright © 2005 John Wiley & Sons, Ltd.     

含有不同脂肪环胺侧基的聚丙烯酰胺保护的贵金属胶体制备的研究

<正> 近年来高分子保护金属胶体的研究在金属催化剂领域中受到人们的突出关注。自Hirai等人对聚乙烯吡咯烷酮保护的铂族金属胶体的系统研究工作发表之后,一项重要的研究进展是双金属胶体的制备成功。当前制备窄分布乃至单分散胶体的努力成为众多研究的集中目标,具有重要的理论意义和实际应用价值。Bradley等报道用金属蒸汽冷凝至含有高分子稳定剂的有机溶剂中制备得到2.0—5.0nm直径的金属胶体,Schmid等报道用水溶性三苯膦磺酸钠小分子配位体作为稳定剂制备得到直径为18.6±0.1nm的金胶体。Esumi等用在有机溶剂中热解乙酸钯的方法制备得到不同粒径的均一球形的钯金属胶体。     

Influence of hydrodynamic coupling on the density dependence of quasi-one-dimensional diffusion

The effect on the short time one particle diffusion coefficient of hydrodynamic interaction between pairs of colloid particles, and between colloid particles and the walls of a quasi-one-dimensional cylindrical channel, are calculated using the method of reflections. The nonzero size of the colloid particle is accounted for in the analysis, and the theoretical predictions are compared with the experimental data of Lin, Cui, Lee, and Yu for the short time one particle diffusion coefficient of colloids in a square open channel [Europhys. Lett. 57, 724 (2002)].     

Probing particle size distributions in natural surface waters from 15 nm to 2 microm by a combination of LIBD and single-particle counting

We present a technique for measuring colloid size distributions between 15 nm and 2 microm at concentrations relevant to natural surface waters. Two particle-measuring methods are combined: laser-induced breakdown detection (LIBD), which allows the quantification of colloid size distributions below 400 nm, and a commercial single-particle counter that extends the accessible size range up to two mum. Centrifugation was used in order to separate micrometer sized particles for the LIBD measurement. The feasibility is demonstrated on water of Lake Brienz (Switzerland) and the River Pfinz (Germany) and the particle size distributions follow Pareto's law even down to 15 nm in both cases.     

Colloid stability of sodium dihexadecyl phosphate/poly(diallyldimethylammonium chloride) decorated latex

The colloid stability of supramolecular assemblies composed of the synthetic anionic lipid sodium dihexadecyl phosphate (DHP) on cationic poly(diallyldimethylammonium chloride) (PDDA) supported on polystyrene sulfate (PSS) microspheres was evaluated via turbidimetry kinetics, dynamic light scattering for particle sizing, zeta-potential analysis, and determination of DHP adsorption on PDDA-covered particles. At 0.05 g/L PDDA and 5 x 10(9) PSS particles/mL, PDDA did not induce significant particle flocculation and a vast majority of PDDA covered single particles were present in the dispersion so that this was the condition chosen for determining DHP concentration (C) effects on particle size and zeta-potentials. At 0.8 mM DHP, charge neutralization, maximal size, and visible precipitation indicated extensive flocculation and minimal colloid stability for the DHP/PDDA/PSS assembly. At 0.05 g L(-1) PDDA, isotherms of high affinity for DHP adsorption on PDDA-covered particles presented a plateau at a limiting adsorption of 135 x 10(19) DHP molecules adsorbed per square meter PSS which was well above bilayer deposition on a smooth particle surface. The polyelectrolyte layer on hydrophobic particles was swelled and fluffy yielding ca. 6 +/- 1.5 nm hydrodynamic thickness. Maximal and massive adsorption of DHP lipid onto this layer produced polydisperse DHP/PDDA/PSS colloidal particles with low colloid stability and which, at best, remained aggregated as doublets over a range of large lipid concentrations so that it was not possible to evaluate the mean total thickness for the deposited film. The assembly anionic lipid/cationic PDDA layer/polymeric particle was relatively stable as particle doublets only well above charge neutralization of the polyelectrolyte by the anionic lipid, at relatively large lipid concentrations (above 1 mM DHP) with charge neutralization leading to extensive particle aggregation.     

Synthesis and optical property of beta-brass colloid

Cu/Zn beta-phase alloy (beta-brass) colloid was successfully synthesized by reducing the organometallic complexes in the organic liquid phase. It was confirmed by X-ray diffraction that the material formed pure beta-phase. The morphology for the beta-brass particles was observed using transmission electron microscopy (TEM). The dispersion of the particle diameter was almost single modal, and the diameter was estimated at 8+/-2 nm. A clear peak around 520 nm was seen in the optical absorption spectrum for the beta-brass colloid, and it is attributed to the surface plasmon absorption. We also simulated the optical absorption spectrum using the bulk dielectric constant for beta-brass. The simulation qualitatively reproduced the experimental data well.     

PICA法制备用于高效液相色谱的锆胶基质柱填料

迄今 ,硅胶基质固定相在 HPLC领域仍占据主导地位 ,但由于它的 p H使用范围窄 ,尤其在碱性条件下基质逐渐溶解 ,其使用受到限制 [1] .为此 ,寻找稳定性能高的新基质成为当前色谱学研究的热点之一 ,二氧化锆因具有良好化学稳定性和机械强度而受到关注 .目前 ,制备微米级、球形和多孔二氧化锆基质柱填料的常用方法有两种 :(1 )油乳化法 (OEM) ;(2 )聚合诱导胶体凝聚法 (PICA) .OEM法操作简单 ,但制备的二氧化锆微球粒径分布宽且孔径较小 .Carr[2 ,3] ,Unger[4 ] ,Rassi[5,6 ]和 Kawahara等[7,8] 在用 OEM法制备二氧化锆微球方面做了…     

Size Effect of Colloidal Selenium Particles on the Inhibition of LPS‐Induced Nitric Oxide Production

We have studied the size‐dependent inhibition capabilities of colloidal selenium (Se) particles on lipopolysaccharide (LPS)‐induced nitric oxide (NO) production in RAW 264.7 cells. Four particle sizes of the nano‐Se, ranging from 45 ? 220 nm in diameter, were examined. All of them, unlike their bulk material, show clear capabilities of inhibition and a trend dependent on the particles size. The inhibition becomes more potent as the particle size increases. It indicates that pursuing the reduction of colloidal sizes into nanoscale is not favoured in this biological system.     

Laser photolysis of silver colloid prepared by citric acid reduction method

By irradiating a silver colloid, prepared via the citric reduction method, using the second harmonic of a Nd:YAG laser, lambda = 532 nm, with laser fluence more than about 0.2 J/cm(2), we prepared a colloid consisting of small spherical silver nanoparticles with d(p) = 8 nm. The process of particle formation can be divided into three steps. First, large particles that existed in the initial colloid evaporate fully, producing a large amount of silver atoms. Next, primary particles with d(p) = 2-4 nm are formed in mini plumes. Finally, these primary particles grow up to 8 nm, as silver atoms diffuse to them through water.     

Dynamic properties of the AgI-solution interface: Implications for colloid stability

This paper discusses the dynamics (i.e. the rates of the various charge displacement processes) of electrical double layers after disequilibration, taking the AgI-electrolyte solution interface as the model system. Relaxation studies performed with Ag/AgI electrodes lead to the conclusion that there is a relatively slow step, connected with the transfer of charge through the solid-solution interface. Evidence is given that this step occurs also with colloidal particles under interaction. It is inferred that in AgI sols interaction takes place at constant total particle charge, but at variable charge density distribution. The effect of particle radius a is also considered, an important parameter being the ratio τ_l/τ_int between the characteristic time scales of lateral charge flow and interaction. This ratio is dominated by the hydrodynamic drag. It appears that these dynamic factors level off the effect of the particle radius on the rate of coagulation. Other implications for colloid stability are discussed.