Effective electrokinetic field-amplified sample injection occurring at the capillary inlet from a sample volume equivalent exceeding that of the capillary up to 10-fold is described and demonstrated to provide over 1000-fold sensitivity enhancement. Successful application of this head-column field-amplified sample stacking approach to the analysis of positively chargeable, hydrophobic compounds in binary system capillary electrophoresis is shown to require an initially introduced low-conductivity zone (water plug) of >1 mm length, a sample injection voltage <20 kV, and an injection time interval <60 s. Following these conditions for more than 1500 runs with capillaries of 50 μm i.d. and about 20 cm effective length, damaging heat production during electroinjection within the low-conductivity zone at the column inlet (boiling of solvent and possible deposition of solutes or fusing of capillary walls) could be prevented. The solute amount injected by head-column field-amplified sample stacking is further shown to be dependent on the organic fraction and the buffer in the sample solution. High content of organic solvent, low conductivity, and the presence of a small amount of H(+) (50-100 μM) provides the highest sensitivity for analysis of positively chargeable model substances, including amiodarone and desethylamiodarone. Solutes present at the nanomolar level can thereby be accumulated from a sample volume equivalent of about 4 μL (with injection of about 20 nL of sample solvent into the capillary) and measured by UV absorption detection. To prevent disturbances caused by electrolysis, sample vials should be employed only once. The data obtained further show that quantitation can be reliably performed using internal calibration based on peak height (RSDs for inter- and intraday determinations are on the 2% level). However, due to variation of the roughness of the capillary walls and cuts, the time interval between operational steps, and trace adsorption onto the capillary walls, the length of the water zone drawn by capillary action on the inlet side is not constant, and external calibration therefore cannot be employed for quantitation.

A new dynamic computer model permitting the combined simulation of the temporal behavior of electroosmosis and electrophoresis under constant voltage or current conditions and in a capillary which exhibits a pH-dependent surface charge has been constructed and applied to the description of capillary zone electrophoresis, isotachophoresis, and isoelectric focusing with electroosmotic zone displacement. Electroosmosis is calculated via use of a normalized wall titration curve (mobility vs pH). Two approaches employed for normalization of the experimentally determined wall titration data are discussed, one that considers the electroosmotic mobility to be inversely proportional to the square root of the ionic strength (method based on the Gouy-Chapman theory with the counterion layer thickness being equal to the Debye-Hückel length) and one that assumes the double-layer thickness to be the sum of a compact layer of fixed charges and the Debye-Hückel thickness and the existence of a wall adsorption equilibrium of the buffer cation other than the proton (method described by Salomon, K.; et al. J. Chromatogr. 1991, 559, 69). The first approach is shown to overestimate the magnitude of electroosmosis, whereas, with the more complex dependence between the electroosmotic mobility and ionic strength, qualitative agreement between experimental and simulation data is obtained. Using one set of electroosmosis input data, the new model is shown to provide detailed insight into the dynamics of electroosmosis in typical discontinuous buffer systems employed in capillary zone electrophoresis (in which the sample matrix provides the discontinuity), in capillary isotachophoresis, and in capillary isoelectric focusing.

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Micellar electrokinetic capillary chromatography (MECC) separations and analyses of biological samples on a planar glass microchip capillary electrophoresis device with laser-induced fluorescence solute detection are discussed. A cyclic channel system which permits dead volume free repeated column switching and thus the use of various channel lengths together with a relatively low applied separation voltage is described. It features an unbiased, dead volume free electrokinetic sample inlet system of approximately 12 pL. Because of the small cross section and favorable heat dissipation in glass microstructures, MECC separations with an electric field strength of up to 2000 V/cm achieving efficiencies of submicrometer plate heights can be performed. After a separation length of 2 cm, six fluorescein isothiocyanate labeled amino acids are shown to be separable within a few seconds and with an imprecision for peak areas (or heights) and detection times of < 2% and < 0.5%, respectively. Without application of electrokinetic solute stacking, the detection limit of fluorescein isothiocyanate labeled arginine is 3.3 nM, corresponding to approximately 40 zmol injected. Furthermore, the feasibility of directly applying human urine and serum samples onto the uncoated channel system is demonstrated and first data of the successful performance of a chip-based MECC immunoassay for serum theophylline are presented. Compared to MECC in conventional fused-silica capillaries, MECC analyses on microchips can be performed 1-2 orders of magnitude faster, with higher efficiency and at no expense of accuracy and precision. Furthermore, versatility is shown to be much increased with the use of a cyclic rather than a single-path channel system. The MECC separation efficiency of fluorescein isothiocyanate labeled amino acids is shown to be comparable to that obtained by gel electrophoresis performed in the same chip layout.

Poly(dimethylsiloxane) (PDMS) appeared recently as a material of choice for rapid and accurate replication of polymer-based microfluidic networks. However, due to its hydrophobicity, the surface strongly interacts with apolar analytes or species containing apolar domains, resulting in significant uncontrolled adsorption on channel walls. This contribution describes the application and characterization of a PDMS surface treatment that considerably decreases adsorption of low and high molecular mass substances to channel walls while maintaining a modest cathodic electroosmotic flow. Channels are modified with a three-layer biotin-neutravidin sandwich coating, made of biotinylated IgG, neutravidin, and biotinylated dextran. By replacing biotinylated dextran with any biotinylated reagent, the modified surface can be readily patterned with biochemical probes, such as antibodies. Combination of probe immobilization chemistry with low nonspecific binding enables affinity binding assays within channel networks. The example of an electrokinetic driven, heterogeneous immunoreaction for human IgG is described.

A 150-component, dynamic electrophoresis simulator was developed and applied to the description of capillary isoelectric focusing (CIEF) of amphoteric substances in quiescent solution. The simulator is shown to be capable of producing high-resolution pH 3-10 focusing data with 140 individual carrier ampholytes (20/pH unit) and at current densities that are used in CIEF, i.e., under conditions that were hitherto unaccessible by dynamic computer simulation. Having a focusing capillary of 5-cm length, the predicted focusing dynamics for amphoteric dyes obtained at a constant voltage of 1500 V (300 V/cm) are shown to qualitatively agree with data obtained by whole-column optical imaging. The simulation data provide detailed insight into the dynamics of the focusing process for the cases with the focusing column being sandwiched between 40 mM NaOH (catholyte) and 100 mM phosphoric acid (anolyte) or having the column ends only permeable for OH- and H+ at cathode and anode, respectively. Simulation data reveal that the number of sample boundaries migrating from the two ends of the column to the focusing positions is always equal to the number of sample components. The number of detectable migrating sample boundaries, however, can be lower. Whole-column optical imaging is demonstrated to be the method of choice for following the approach to equilibrium. With that detection format, transient sample peaks can be recognized and properly identified. This would also be possible with a scanning detector moving rapidly and repeatedly along the column but cannot be accomplished by a stationary detector placed at a specified location. The data presented demonstrate that the model together with imaging monitoring can be used to optimize the CIEF separation conditions.

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