硅胶电色谱分离机理的研究

对硅胶电色谱柱的性能进行了考察,发现在水／有机溶剂流动相条件下,几乎不存在气泡问题,流动相的组成在有机溶剂浓度、电解质浓度、ＰＨ值等方面可以在较大范围变化,选用５种典型样品,对硅胶电色谱的分离机理进行了系统研究,发现有反相分离机理、正相吸附机理、离子交换机理以及电泳机理参与作用。同时考察了有机溶剂浓度、电解质浓度、ＰＨ等对分离的影响。此外,还首次提出了一种全新的电色谱模式－动态改性硅胶电色谱。     

反相毛细管电色谱电渗流影响因素的研究

在７５μｍ×２０ｃｍ的毛细管ＯＤＳ填充柱上实现毛细管反相电色谱分离，考察种种分离因素，包括流动相的组成，有机相的种类和比例，电解质缓冲液的种类浓度和ＰＨ值，以及分离电压和分离温度等因素对填充毛细管电渗流的影响，系统研究了反相毛细管电色谱的电渗变化规律。     

在不同体积比流动相及不同缓冲溶液中毛细电色谱ODS柱的分离行为

１引言毛细电色谱中，流动相的选择同样取决于固定相及被分离样品。对于ＯＤＳ柱，若分离中性样品时，通常选择一定体积比的有机相和无机缓冲溶液混合，如一定百分比的ＣＨ３ＣＮ和一定百分比的Ｎａ２Ｂ４Ｏ７水溶液。流动相浓度配比不同时，样品在固定相上的保留不同，进而造成分离时间和选择性不同。笔者通过实验观察到，当在同样浓度的有机相中加入的缓冲溶液不同时，固定相对样品的分离能力也不尽相同。本文即以实验为依据，分别讨论ＯＤＳ柱在不同体积比流动相及在相同体积比流动相，不同缓冲溶液下的分离行为。２实验部分２．１仪器与…     

石英砂整体微柱的制备及其反相电色谱分离研究

在2.2mm内径的石英管中,采用正硅酸四乙酯水解的溶胶-凝胶法合成了填充细石英砂的高比表面积电色谱整体柱,并用正辛基三乙氧基硅烷键合制备反相色谱固定相.填充细石英砂的电色谱整体柱抑制了大柱径引起的电流热效应,采用电渗流驱动流动相,分离了苯酚和苯,实验证明该整体微柱用于电色谱分离和改善浓度检出限的可行性.     

液相色谱塔板高度方程的统一形式

研究了色谱分离过程中物质的径向扩散和流动相发热对柱效能的影响。从热传导方程出发,运用色谱过程动力学原理推导了包括考虑流动相径向扩散、色谱柱发热影响的液相色谱塔板高度方程：

该方程概括了高效液相色谱（HPLC）、超高效液相色谱（UPLC）、毛细管电色谱（CEC）和消滞留层液相色谱（ESFLC）塔板高度与各种因素的关系。方程最后一项代表了径向扩散和柱发热对塔板高度的贡献。当流动相线速度较低且柱内径较细时,流动相摩擦生热和径向扩散对塔板高度的贡献趋近于零,塔板高度方程还原成Horvath和Lin的方程;当流动相线速度较高时,由于流动相摩擦生热,柱轴心与边缘温差增加,导致流动相线速度径向分布差异,使得柱效率降低。柱轴心与边缘的温差与流动相线速度平方成正比。该文指出,在流动相高线速度情况下,液相色谱的柱效率与柱内径密切相关,采用细内径柱有利于实现高速与高效率;过高的流动相线速度将导致色谱柱效率崩溃。     

聚羧酸系减水剂的大单体组分的分离分析

采用高效液相色谱-电喷雾式检测器分离分析聚羧酸系减水剂的大单体组分-脂肪醇聚氧乙烯基醚类。以Agilent ZORBAX SB-C8柱为分离柱,甲醇-水溶液为流动相进行梯度洗脱,采用电喷雾式检测器。在优化的色谱条件下,样品各组分间分离效果良好。高效液相色谱-质谱联用分析结果表明,各组分依据大单体中EO加合数的不同进行分离。     

非极性毛细管电色谱原位柱的阳离子表面活性剂动态修饰

毛细管电色谱是在毛细管中依靠电渗流来驱动流动相 ,同时溶质与固定相发生相互作用的一种色谱分离模式 ,它有高效液相色谱的高选择性 ,同时兼具毛细管电泳的高效性 [1] .传统电色谱柱是将HPLC填料装入毛细管 ,但由于装柱困难且易产生气泡而在一定程度上阻碍了电色谱的发展 [2～ 4 ] .通过柱内合成的方法直接在毛细管中制成连续床毛细管电色谱柱 ,可避免两端烧塞 . 1 995年 Svec等 [5,6]首次将连续床层色谱柱用于毛细管电色谱 ,此后 ,有关毛细管中原位合成连续床电色谱柱的方法得到了应用 [7～ 11] .为了使原位合成电色谱柱能产生电渗流 ,…     

320 μm内径毛细管电色谱柱的分离条件研究

在毛细管电色谱中，随着柱径的加粗，焦耳热效应使柱效急剧降低，甚至产生气泡，导致断流现象；采用有机盐缓冲溶液作为流动相，在320μm内径反相毛细管柱中成功地使几种苯取代物得到较好的分离，并且可以在较高的电压下操作，得到了比加压电色谱法更高的柱效。通过对选择缓冲溶液的讨论，说明了大内径毛细管柱中调节流动相组成的一般原则。     

分散固相萃取结合高效液相色谱-串联质谱快速测定茶叶中的苦参碱

建立了茶叶中苦参碱残留量的分散固相萃取-液相色谱-串联质谱检测方法。样品经氨水碱化，乙腈提取，浓缩后经分散固相萃取净化，以乙腈和乙酸铵溶液为流动相进行梯度洗脱，C18色谱柱分离，采用电喷雾离子源，正离子扫描，多反应监测(MRM)模式测定，外标法定量。结果表明，苦参碱在1.0～20 ng/mL范围内线性关系良好，相关系数大于0.998。方法对于茶叶中苦参碱的定量限为5.0μg/kg。在5.0、10和50μg/kg 3个加标浓度水平下的加标回收率为80%～98%,相对标准偏差均不大于7.2%。本方法快速、简便，准确性和灵敏度较高，可作为茶叶中苦参碱残留量的有效检测方法。     

多肽的反相梯度加压毛细管电色谱分离

以C18为固定相，采用电压和压力联合驱动流动相，研究反相加压毛细管电色谱分离多肽；考察了加压电色谱中，电压对带电和中性物质迁移的影响，实现了梯度加压毛细管电色谱分离6种多肽；结果表明，加压电色谱可以很好地抑制气泡形成，实验结果准确，重复性好；梯度加压毛细管电色谱在复杂样品的分离分析中，具有很大的潜力。     

毛细管反相电色谱法分离行为的研究

对乙睛-水-磷酸二氢销体系毛细管反相电色谱分离行为进行了研究。采用柱上紫外检测,在75μmi.d.×30cm的毛细管ODS（3μm）填充柱上获得了小于2.0的折合培板高度。同时还研究了乙睛的比例、电解质的浓度和电场强度等因素对电渗流和往效的影响。     

Some considerations concerning the composition of the mobile phase in capillary electrochromatography

In capillary electrochromatography (CEC) the propulsion of the mobile phase is effected by electroosmosis. The velocity of the electroosmotic flow is dependent on surface properties of the stationary phase and on bulk properties of the mobile phase. Therefore, in CEC the optimization of the mobile phase composition must take more factors into account than in pressure-driven LC. In this paper, the impact of the electrolyte concentration in the mobile phase and of the volume fraction of the organic mobile phase constituent on the velocity of the electroosmotic flow and on the chromatographic efficiency is investigated for CEC with capillaries packed with octadecylsilica gel. Bias of the data by an open section of the capillary has been excluded by employing completely packed capillaries and detection in a packed section. Acetonitrile as organic constituent of the mobile phase is compared to other possible organic modifiers (polar organic solvents) concerning influence on velocity of the electroosmotic flow and retention of solutes.     

Separation of enantiomers by packed capillary electrochromatography on a cellulose-based stationary phase

Separation of enantiomers was performed by applying packed capillary electrochromatography (CEC). Fused-silica capillaries of different lengths with an inner diameter of 100 microm were packed with a cellulose derivative immobilized onto macroporous silica gel. Parameters such as content of modifier in the mobile phase, concentration and pH of the buffer were varied for a set of test capillaries to determine their influence on enantioselectivity. In packed CEC the highest influence on resolution of the test racemates was found by changing the acetonitrile content, while variation of the buffer concentration mostly affects the electroosmotic velocity. The performance of packed CEC and nano-LC was also compared. Packed CEC showed much better column efficiency and enantioselectivity under similar flow/electroosmotic velocity.     

In-line coupling of low-pressure short capillary electrochromatography columns to electrospray ionisation mass spectrometry

A new in-house designed and constructed injection valve for capillary electrochromatography (CEC) based on a rotating injection part with compartments for the eluent as well as for the sample has been coupled to a mass spectrometer via a sheath flow electrospray ionisation (ESI) interface, using short capillary columns of 15 cm length. The CEC columns were packed with 3 microm C(18) bonded silica particles, and a mixture of peptides was analysed using an ammonium acetate/acetonitrile eluent. A significant increase in the signal-to-noise ratio was obtained when the peptides were dissolved in water with the same content of organic modifier as in the eluent with an addition of 0.5% (v/v) acetic acid. When the CEC analysis was performed without any additional pressure, the separation current sometimes dropped tremendously due to bubble formation, caused by different permeability in the first and packed part of the column causing an extremely low electroosmotic flow. The separation current was restored to its original value by applying only 7 bar at the inlet of the CEC column, and the separation performance for the test peptides was recovered. A comparison of the CEC performance of peptides in pure CEC mode and in low-pressure CEC mode is reported.     

Capillary electrochromatography using fibers as stationary phases.

Fiber-packed capillary columns have been evaluated in chromatographic performance in capillary electrochromatography (CEC). The change of electroosmotic flow (EOF) velocity and selectivity using different kinds of fiber materials was examined. Although the EOF velocity among the different fiber packed columns was almost the same, retention of parabens was larger on the Kevlar-packed column than on the Zylon-packed one, and was larger on the as-span-type fiber-packed column than on the high-modulus-type packed one. Using 200 microm ID x 5 cm Kevlar packed column combined with a 100 microm ID x 20 cm precolumn capillary and a 530 microm ID x 45 cm postcolumn capillary, the separation of three parabens within 30 s was achieved. Other compounds were also separated in a few minutes by the fiber-packed CEC method.     

Modeling the velocity field of the electroosmotic flow in charged capillaries and in capillary columns packed with charged particles: interstitial and intraparticle velocities in capillary electrochromatography systems

Mass transfer systems based on electrokinetic phenomena (i.e., capillary electrochromatography (CEC)) have shown practical potential in becoming powerful separation methods for the biotechnology and pharmaceutical industries. A mathematical model has been constructed and solved to describe quantitatively the profiles of the electrostatic potential, pressure, and velocity of the electroosmotic flow (EOF) in charged cylindrical capillaries and in capillary columns packed with charged particles. The results obtained from model simulations (i) provide significant physical insight and understanding with regard to the velocity profile of the EOF in capillary columns packed with charged porous particles which represent systems employed in CEC, (ii) provide the physical explanation for the experimental results which indicate that the velocity of the EOF in capillary columns packed with charged porous particles is a very weak function (it is almost independent) of the diameter of the particles, and (iii) indicate that the intraparticle velocity, nu(p,i), of the EOF can be greater than zero. The intraparticle Peclet number, Pe(int rap), for lysozyme was found to be greater than unity and this intraparticle convective mass transfer mechanism could contribute significantly, if the appropriate chemistry is employed in the mobile liquid phase and in the charged porous particles, in (a) decreasing the intraparticle mass transfer resistance, (b) decreasing the dispersive mass transfer effects, and (c) increasing the intraparticle mass transfer rates so that high column efficiency and resolution can be obtained. Furthermore, the results from model simulations indicate that for a given operationally permissible value of the applied electric potential difference per unit length, Ex, high values for the average velocity of the EOF can be obtained if (1) the zeta potential, zeta(p), at the surface of the particles packed in the column has a large negative magnitude, (2) the value of the viscosity, mu, of the mobile liquid phase is low, (3) the magnitude of the dielectric constant, epsilon, of the mobile liquid phase is reasonably large, and (4) the combination of the values of the concentration, C(infinity), of the electrolyte and of the dielectric constant, epsilon, provide a thin double layer. The theoretical results for the velocity of the EOF obtained from the solution of the model presented in this work were compared with the experimental values of the velocity of the EOF obtained from a fused-silica column packed with charged porous silica C8 particles. Systems with four different particle diameters and three different concentrations of the electrolyte were considered, and the magnitude of the electric field was varied widely. The agreement between theory and experiment was found to be good.     

Life-time studies with capillary electrochromatography columns operated under different conditions

A test system has been established to permit the monitoring of the life-time performance of several reversed- phase capillary electrochromatography (CEC) columns. The retention factors, k(cec), peak symmetry coefficients, lambda(sym), and column efficiencies, N, of three neutral n-alkylbenzene analytes, namely ethyl-, n-butyl- and n-pentylbenzenes, were determined for Hypersil 3 microm n-octylsilica and n-octadecylsilica packed into CEC capillary columns of 100 microm I.D., with a packed length of 250 mm, and a total length of 335 mm. The performances of these CEC capillary columns were examined for a variety of eluents with pH values ranging between pH 2.0 - 8.0, similar to those employed to study the retention behaviour of peptides that we have previously reported. The relative standard deviation (RSD) of the retention factors (k(cec) values) of these n-alkylbenzenes, acquired with an eluent of (25 mM Tris-HCl, pH 8.0,)-acetonitrile (1:4, v/v), when the CEC capillary columns were used for the first time (virgin values), were 4% (based on data acquired with 4 CEC capillary columns) for the n-octyl bonded silica capillary columns, and 6% (based on 8 columns) for n-octadecyl bonded silica capillary columns. The RSD values of the k(cec) values of the n-alkylbenzenes for one set of replicates (n=6) with one CEC capillary column was < 0.5%. The theoretical plate numbers, N, for the virgin CEC capillary columns were ca. 60,000, whilst the observed N values for all new CEC capillary columns were > or = 40,000 for n-octyl bonded silica capillary columns and > or = 50,000 for n-octadecyl bonded silica capillary columns. The peak symmetry coefficients, lambda(sym), of the n-alkylbenzenes for virgin CEC capillary columns and for CEC capillary columns used for more than 1,000 injections were always in the range 0.95-1.05. The experimental results clearly document that the life-time performance of the CEC capillary columns depends on the eluent composition, as well as the nature of the analytes to which the CEC capillary columns are exposed.     

毛细管电色谱和加压毛细管电色谱的进展与应用

毛细管电色谱(CEC)以内含色谱固定相的毛细管为分离柱,以电渗流为驱动力,既可以分离带电物质也可以分离中性物质。它结合了毛细管电泳和高效液相色谱两者的优点,兼具高柱效、高分辨率、高选择性和高峰容量的特点,同时具有色谱和电泳的双重分离机理。然而,“纯粹”的电色谱在实际应用中有着天然的弱点,即: 在电流通过毛细管柱中的流动相时容易产生气泡(焦耳热作用),从而使电流中断和电渗流停止,毛细管柱必须被重新用流动相润湿后方能再次使用。加压毛细管电色谱(pCEC)将液相色谱中的压力流引入CEC系统中,不仅解决了气泡、干柱等问题,而且实现了定量阀进样和二元梯度洗脱。CEC和pCEC作为微分离领域的两种前沿技术,满足了当前复杂样品分析和分析仪器微型化的需求,近年来获得了广泛的关注。本文综述了这两种技术近来的发展,包括仪器、色谱固定相的发展,总结了其在生命科学、药物分析、食品安全以及环保样品分析等方面的应用进展,评述了各方法的特点,并展望了CEC和pCEC今后的发展和应用前景。     

Evaluation of ODS-AQ stationary phase for use in capillary electrochromatography

The aim of this study was to evaluate the applicability of ODS-AQ packing material as a stationary phase in capillary electrochromatography (CEC). The electroosmotic flow created on an ODS-AQ stationary phase was measured at different mobile phase compositions and at different column temperatures. It was observed that the electroosmotic flow generated in the column increased by 50% when the temperature of the system was raised from 20 degrees C to 60 degrees C, while all other conditions were kept constant. The electroosmotic flow produced by the ODS-AQ stationary phase was found to be comparable to the flow generated in a column packed with Nucleosil bare-silica material. In addition, a set of polar compounds (D-lysergic acid diethylamide derivatives) was utilized to determine the influence of temperature and mobile phase composition on their chromatographic behavior on an ODS-AQ stationary phase in a CEC mode. A linear relationship between the solute retention factor and column temperatures was seen over the temperature range studied (20 degrees C to 60 degrees C). A quadratic function was used to describe the changes in the solute retention factors with variation of acetonitrile concentration in the mobile phase.     

Electrohydrodynamics in hierarchically structured monolithic and particulate fixed beds

We have investigated the basic dependence of electroosmotic flow (EOF) velocity and hydrodynamic dispersion in capillary electrochromatography (CEC) on the variation of applied field and mobile phase ionic strengths employing silica-based particulate and monolithic fixed beds. These porous media have a hierarchical structure characterized by discrete intraparticle (intraskeleton) mesoporous and interparticle (interskeleton) macroporous spatial domains. While the macroporous domains contain quasi-electroneutral electrolyte solution, the ion-permselectivity (charge-selectivity) of the mesoporous domains determines the co-ion exclusion and counter-ion enrichment at electrochemical equilibrium (without superimposed electrical field) which depends on mesopore-scale electrical double layer (EDL) overlap and surface charge density. This adjustable, locally charge-selective transport realized under most general conditions forms the basis for concentration polarization (CP) induced by electrical fields superimposed in CEC. CP characterizes the formation of convective diffusion boundary layers with reduced (depleted CP zone) and increased (enriched CP zone) electrolyte concentration, respectively, at the anodic and cathodic interfaces in fixed beds containing the cation-selective, silica-based particles (or monolith skeleton). CP originates in the electrical field-induced coupled mass and charge transport normal to the charge-selective interfaces and has consequences for the EOF dynamics, hydrodynamic dispersion, and analyte retention in CEC. A secondary EDL with mobile counter-ionic space charge can be induced in the depleted CP zone leading to induced-charge EOF in the macroporous domains. It is characterized by a nonlinear dependence of the average EOF velocities on applied field strength and strong local velocity components tangential to the surface which enhance lateral pore-scale dispersion, thereby decreasing (axial) zone spreading. Differences in the pore space morphology of random-close sphere packings and monoliths criticially affect the intensity of CP and induced-charge EOF in these materials. CP is identified as a key phenomenon in CEC which also influences effective migration and the retention of charged analytes because the local intensity of CP inherently depends on applied field and mobile phase ionic strengths.