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            but is also provides plug flow through the column, as opposed to the parabolic velocity profile normally
            associated with fluid-flow through tubes. The lack of a parabolic velocity profile can have a dramatic
            effect on the column efficiency, as shown in Chapter 1. One of the early reports on the successful use of
            electrosmotic flow in LC, was that of Schmeer et al. [12], and the layout of their apparatus is depicted
            in Figure 13.14.

























                                                         Figure 13.14
                                           The Capillary Electrochromatography Apparatus

            Electro-osmotic flow is obtained by applying a strong electric field across the length of the column. The
            velocity of the flow is independent of the particle size of the packing, and so columns 0.5 mm in
            diameter, packed with particles 1.2 µm in diameter, can readily be used if so desired. Employing
            columns of this diameter, packed with such small particles, efficiencies of 200,000 theoretical plates
            can easily be obtained. In practice, to minimize resistance heating, columns of 50 to 100 µm I.D. are
            usually employed, with flow rates up to 2 µl/min. This magnitude of the flow rate is ideal for
            electrospray nebulizing and consequently, no sheath flow is necessary. However, in order to assure
            stable flow conditions a supplementary flow of mobile phase was provided by a mechanical pump as
            shown in Figure 13.13. The fused capillary column 20 cm long, 100 µm I.D., and 360 µm O.D., was
            fitted with a terminal fused silica gel frit
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