非对称场流分离技术在蛋黄浆质低密度脂蛋白粒径表征中的应用

通过自组装的非对称场流分离系统(AF4)与紫外可见光检测器联用分离表征了笼养鸡蛋、柴鸡蛋、鹌鹑蛋和鸭蛋蛋黄浆质中的低密度脂蛋白(LDL)。在近似蛋黄浆质生理条件下,研究了进样量、交叉流流速、膜的类型对AF4蛋黄浆质中LDL分离表征的影响;考察了该方法的精密度。在优化的AF4分析条件下,检测出了笼养鸡蛋、柴鸡蛋、鹌鹑蛋和鸭蛋蛋黄浆质中LDL的水力学粒径分布。LDL的AF4洗脱峰高和峰面积的日内精密度分别为1.3%和1.9%(n=7),日间精密度分别为2.4%和2.3%(n=7)。研究结果表明,该方法可用于分离禽类蛋黄浆质中的LDL,同时能够得到LDL水力学粒径分布。     

非对称场流分离技术用于纳米颗粒的表征

采用非对称场流分离技术(Asymmetrical flow field-flow fractionation,AF4)对标准聚苯乙烯颗粒粒径进行表征。利用非对称场流分离仪以0.1%SDS(十二烷基磺酸钠)和0.02%NaN3的水溶液为流动相,测定标准的聚苯乙烯纳米颗粒在流体流场作用下通过分离腔室的保留时间,以确定纳米颗粒的平均粒径。优化了聚焦时间、横向流速、进样量、主体流速等实验条件,建立了利用AF4准确表征纳米颗粒的方法,并与扫描电镜(Scanning electron microscope,SEM)的表征结果进行比较。结果表明,AF4的表征结果比SEM更接近于聚苯乙烯颗粒的标准粒径,具有更高的稳定性和准确度。本方法可作为纳米粒径表征的一种准确方法。     

基于非对称场流分离技术分离表征小米淀粉

基于非对称场流分离技术耦合多角度激光光散射检测器和示差折光检测器,建立了分离表征小米淀粉的方法。研究了进样量、交叉流流速、半衰期（t_1/2）、载液离子强度和pH值对小米淀粉分离效果的影响;考察了该方法的重现性;探究了小米淀粉分子结构。结果表明,在进样体积为50 μL、进样质量浓度为0.50 g/L、交叉流流速为1.2 mL/min、t_1/2=3 min、载液为10 mmol/L pH 7.00 NaNO₃（含3 mmol/L NaN₃）的条件下,小米淀粉分离效果最佳。该方法具有良好的重现性,得到的小米淀粉的回转半径相对标准偏差为3.4%、摩尔质量相对标准偏差为7.0%。     

非对称流场流分离技术在纳米材料及生物分子表征方面的应用

场流分离作为一类分离技术可分离、提纯和收集流体中的悬浮物微粒,它是将流体与外场联合作用于待分离物质,利用样品质量、体积和密度等性质的差异实现分离,然后利用分离物质的保留性质来确定样品颗粒粒径及分布、分子量等性质。其中非对称流场流分离能够提供连续的、高分辨率的分离,近年来越来越受到科研人员的欢迎。本文介绍了场流分离的分类及其原理,重点介绍了非对称流场流分离的原理及其应用,包括非对称流场流分离的影响因素及与其他分离技术的比较;最后总结了该技术的发展趋势。     

非对称流场流分离技术的现状及发展趋势

场流分离是生物分析领域一项成熟的技术,将流体与外场联合作用于待分离物质,利用分析物某些理化参数上的差异进行分离。非对称流场流是其重要的分支之一,所施加的外力场为垂直方向的液流,分离过程于开放型的通道中在某种组成的载液迁移推动下进行,主要根据分析物与垂直施加的第二维液流之间的相互作用完成分离。非对称流场流在蛋白质、蛋白质复合物、衍生纳米级/微米级粒子、亚细胞单元和聚合物等分离中的应用日益广泛,主要归功于其直接应用于生物样品时可进行无损分离,因此生物分析物如蛋白质可以在生物友好型的环境中完成分离而不改变其构型,也无需使用降解载液。分离设备便于保持无菌状态,分析物可在生物友好的环境中维持其自然状态。该文简要描述了场流分离原理并罗列出其在生物分析领域一些卓越的发展和应用。     

重力场流分离系统用于聚苯乙烯颗粒的分离条件优化

重力场流分离是最简单的场流分离(gravitational flow-field fractionation,GrFFF)技术,常用于分离粒径几微米到几十微米的颗粒及生物样品。利用自组装加工的重力场流分离仪器分离3种不同粒径(3、6、20μm)的聚苯乙烯(PS)颗粒。自制了一种混合表面活性剂,并与商品化的表面活性剂FL-70进行了比较。通过均匀设计优化流速、混合表面活性剂中聚乙二醇辛基苯基醚(Triton X-100)的质量分数、载液黏度、停流时间等分离条件,以分离度(Rs)和保留比(R)为评价指标,发现FL-70的分离效能略优于自制的混合表面活性剂,可实现3种PS颗粒的完全分离(Rs1为1.771,Rs2为2.074)。结果表明该系统具有良好的分离性能。     

载液组成对于卵白蛋白在非对称流场流分离通道中膜吸附和聚集行为的影响

非对称流场流分离技术对于蛋白质等生物大分子的分析具有温和、分离范围广的特点。然而,在场流分离通道中,受载液组成的影响而产生的蛋白质与通道膜的相互作用和蛋白质在通道内的聚集行为,会影响分析物的回收率和尺寸形态,这些现象一定程度上限制了场流分离仪器的进一步应用。该文研究了载液组成对于卵白蛋白在非对称流场流分离中膜吸附和聚集行为的影响。考察了不同pH （6.2、7.4、8.2）、阳离子种类（Na⁺、K⁺、Mg²⁺）及多种离子强度（0~0.1 mol/L）等条件对卵白蛋白洗脱过程的影响。结果表明a）载液的离子强度越大,卵白蛋白的吸附和聚集行为越严重;b） pH和蛋白质的等电点pI的相对大小决定了蛋白质的表面电荷,从而影响蛋白质的吸附聚集行为;c）二价阳离子Mg²⁺更易引发通道中蛋白质的吸附和聚集。这些结果有助于今后使用非对称流场流分离技术分析蛋白质样品时,改善载液组成以获得更高的回收率,降低蛋白质聚集作用,对AF4更广泛地应用于蛋白质生化分析中有较好的参考价值。     

重力场流分离系统中载液及流速条件对分离的影响

重力场流分离作为最简单的一种场流分离技术,常用于分离微米级颗粒。选择两种不同粒径(20 μ m和6 μ m)的聚苯乙烯(PS)颗粒作为样品,通过改变载液中叠氮化钠浓度、混合表面活性剂的比例及载液流速,利用自行设计生产的重力场流分离(gravitational flow field-flow fractionation, GrFFF)仪器,对颗粒混合样品进行分离,得到了相关谱图与数据,考察了这3种因素对分离效果(保留比(R)、塔板高度(H))的影响。结果表明:20 μ m PS颗粒的R值均大于6 μ m PS颗粒的R值,H值均小于6 μ m颗粒的H值;PS颗粒的R值与H值均随着载液中叠氮化钠浓度的增加而增加;但随着载液流速的增加,R值增加,H值减小。该研究为GrFFF系统的开发及应用提供了重要的参考价值。     

淀粉衍生物微球的制备及其表征

以可溶性淀粉为原料,环氧氯丙烷(ECH)与N,N-亚甲基双丙烯酰胺分别为交联剂(MBAA),Span 60和Tween 60为乳化剂,环己烷和三氯甲烷混合液为油相,硝酸铈铵为引发剂,反相乳液聚合法合成淀粉衍生物微球.通过红外光谱判定主要官能团的变化,借用图片直观淀粉衍生物微球的形貌,判断其控制聚合变量各种因素对合成微球形貌的影响,找到最佳合成条件为可溶性淀粉浓度5%,交联剂用量3 g,引发剂硝酸铈铵用量0.15g,水油相体积比2∶5,聚合温度65℃,聚合时间2 h.使得聚合衍生微球在形体类似球型,体内多孔多面,为进一步探讨吸附作用完成前期工作.     

Effect of asymmetrical flow field-flow fractionation channel geometry on separation efficiency

The separation efficiencies of three different asymmetrical flow field-flow fractionation (AF4) channel designs were evaluated using polystyrene latex standards. Channel breadth was held constant for one channel (rectangular profile), and was reduced either linearly (trapezoidal profile) or exponentially (exponential profile) along the length for the other two. The effective void volumes of the three channel types were designed to be equivalent. Theoretically, under certain flow conditions, the mean channel flow velocity of the exponential channel could be arranged to remain constant along the channel length, thereby improving separation in AF4. Particle separation obtained with the exponential channel was compared with particle separation obtained with the trapezoidal and rectangular channels. We demonstrated that at a certain flow rate condition (outflow/inflow rate = 0.2), the exponential channel design indeed provided better performance with respect to the separation of polystyrene nanoparticles in terms of reducing band broadening. While the trapezoidal channel exhibited a little poorer performance than the exponential, the strongly decreasing mean flow velocity in the rectangular channel resulted in serious band broadening, a delay in retention time, and even failure of larger particles to elute.     

Carboxymethylation of corn starch and characterization using asymmetrical flow field-flow fractionation coupled with multiangle light scattering

Asymmetrical flow field-flow fractionation (AsFlFFF) was coupled online with multiangle light scattering (MALS) to study the changes in the molecular weight and the size distribution of the corn starch during carboxymethylation. A corn starch was derivatized with sodium chloroacetate in alcoholic medium under alkaline condition to produce carboxymethyl starches (CMS) having various degrees of substitution (DS). The change in thermal characteristics and granule structure of the native corn starch and CMS were compared using Thermogravimetric analysis and scanning electron microscope. The ionic strength of the carrier liquid (water with 0.02% NaN₃) was optimized by adding 50 mM NaNO₃ to minimize the interactions among the starch molecules and between the starch molecules and the AsFlFFF membrane. A field-programmed AsFlFFF allowed determination of the molecular weight distribution (MWD) of starches within about 25 min. It was found that carboxymethylation of starch results in reduction in the molecular weight due to molecular degradation by the alkaline treatment. The weight-average molecular weight (M_w) was reduced down to about 4.4 × 10⁵ from about 7.2 × 10⁶ when DS was 0.14. It seems AsFlFFF coupled with MALS (AsFlFFF/MALS) is a useful tool for monitoring the changes taking place in the molecular weight and the size of starch during derivatization.     

Separation of carbon nanotubes by frit inlet asymmetrical flow field-flow fractionation

Flow field-flow fractionation (flow FFF), a separation technique for particles and macromolecules, has been used to separate carbon nanotubes (CNT). The carbon nanotube ropes that were purified from a raw carbon nanotube mixture by acidic reflux followed by cross-flow filtration using a hollow fiber module were cut into shorter lengths by sonication under a concentrated acid mixture. The cut carbon nanotubes were separated by using a modified flow FFF channel system, frit inlet asymmetrical flow FFF (FI AFIFFF) channel, which was useful in the continuous flow operation during injection and separation. Carbon nanotubes, before and after the cutting process, were clearly distinguished by their retention profiles. The narrow volume fractions of CNT collected during flow FFF runs were confirmed by field emission scanning electron microscopy and Raman spectroscopy. Experimentally, it was found that retention of carbon nanotubes in flow FFF was dependent on the use of surfactant for CNT dispersion and for the carrier solution in flow FFF. In this work, the use of flow FFF for the size differentiation of carbon nanotubes in the process of preparation or purification was demonstrated.     

Thermal aggregation of bovine serum albumin studied by asymmetrical flow field-flow fractionation

The use of asymmetrical flow field-flow fractionation (AsFlFFF) in the study of heat-induced aggregation of proteins is demonstrated with bovine serum albumin (BSA) as a model analyte. The hydrodynamic diameter (d_h), the molar mass of heat-induced aggregates, and the radius of gyration (R_g) were calculated in order to get more detailed understanding of the conformational changes of BSA upon heating. The hydrodynamic diameter of native BSA at ambient temperature was ∼7 nm. The particle size was relatively stable up to 60 °C; above 63 °C, however, BSA underwent aggregation (growth of hydrodynamic diameter). The hydrodynamic diameters of the aggregated particles, heated to 80 °C, ranged from 15 to 149 nm depending on the BSA concentration, duration of incubation, and the ionic strength of the solvent. Heating of BSA in the presence of sodium dodecyl sulfate (1.7 or 17 mM) did not lead to aggregation. The heat-induced aggregates were characterized in terms of their molar mass and particle size together with their respective distributions with a hyphenated technique consisting of an asymmetrical field-flow fractionation device and a multi-angle light scattering detector and a UV-detector. The carrier solution comprised 8.5 mM phosphate and 150 mM sodium chloride at pH 7.4. The weight-average molar mass (M_w) of native BSA at ambient temperature is 6.6 × 10⁴ g mol⁻¹. Incubation of solutions with BSA concentrations of 1.0 and 2.5 mg mL⁻¹ at 80 °C for 1 h resulted in aggregates with M_w 1.2 × 10⁶ and 1.9 × 10⁶ g mol⁻¹, respectively. The average radius of gyration and the average hydrodynamic radius of the heat-induced aggregate samples were calculated and compared to the values obtained from the size distributions measured by AsFlFFF. For comparison static light scattering measurements were carried out and the corresponding average molar mass distributions of solutions with BSA concentrations of 1.0 and 2.5 mg mL⁻¹ at 80 °C for 1 h gave aggregates with M_w 1.7 × 10⁶ and 3.5 × 10⁶ g mol⁻¹, respectively.     

Size characterization of drug-loaded polymeric core/shell nanoparticles using asymmetrical flow field-flow fractionation

Asymmetrical flow field-flow fractionation (AsFlFFF) was used to determine the size distribution of drug-loaded core/shell nanoparticles which have a lipid core of lecithin and a polymeric shell of a Pluronic. AsFlFFF provided separation of the drug-loaded core/shell nanoparticles from smaller coreless polymeric micelles, thus allowing accurate size analysis of the drug-loaded nanoparticles without interference by the coreless micelles. It was found from AsFlFFF that the drug-loaded nanoparticles have broad size distributions ranging from 100 to 600 nm in diameter. It was also found that, after the nanoparticles had been stored for 70 days, they disappeared as a result of self-degradation. Being a separation technique, AsFlFFF seems to be more useful than transmission electron microscopy or dynamic light scattering for size analysis of core/shell nanoparticles, which have broad and bimodal size distributions. Figure Separation by AsFlFFF     

Stability of phospholipid vesicles studied by asymmetrical flow field-flow fractionation and capillary electrophoresis

The stability of zwitterionic phosphatidylcholine vesicles in the presence of 20 mol% phosphatidyl serine (PS), phosphatidic acid (PA), phosphatidyl inositol (PI), and diacylphosphatidyl glycerol (PG) phospholipid vesicles, and cholesterol or calcium chloride was investigated by asymmetrical flow field-flow fractionation (AsFlFFF). Large unilamellar vesicles (LUV, diameter 100 nm) prepared by extrusion at 25 °C were used. Phospholipid vesicles (liposomes) were stored at +4 and −18 °C over an extended period of time. Extruded egg yolk phosphatidylcholine (EPC) particle diameters at peak maximum and mean measured by AsFlFFF were 101 ± 3 nm and 122 ± 5 nm, respectively. No significant change in diameter was observed after storage at +4 °C for about 5 months. When the storage period was extended to about 8 months (250 days) larger destabilized aggregates were formed (172 and 215 nm at peak maximum and mean diameters, respectively). When EPC was stored at −18 °C, large particles with diameters of 700–800 nm were formed as a result of dehydration, aggregation, and fusion processes. In the presence of calcium chloride, EPC alone did not form large aggregates. Addition of 20 mol% of negatively charged phospholipids (PS, PA, PI, or PG) to 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylcholine (POPC) vesicles increased the electrostatic interactions between calcium ion and the vesicles and large aggregates were formed. In the presence of cholesterol, large aggregates of about 250–350 nm appeared during storage at +4 and −18 °C for more than 1 day.

The effect of liposome storage temperature on phospholipid coatings applied in capillary electrophoresis (CE) was studied by measuring the electroosmotic flow (EOF). EPC coatings with and without cholesterol, PS, or calcium chloride, prepared from liposomes stored at +25, +4, and −18 °C, were studied at 25 °C. The performances of the coatings were further evaluated with three uncharged compounds. Only minor differences were observed between the same phospholipid coatings, showing that phospholipid coatings in CE are relatively insensitive to storage at +25, +4 °C or −18 °C.