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Separation Power of Steady-State Methods

In isoelectric focusing, as in electrophoresis, the force acting on a species having z elementary charges is zSFE, Eq. 8.8. Charge z, of course, is zero at the isoelectric point, equivalent to the focusing point, y = 0. At positions close to y = 0, z increases as follows [Pg.180]

Velocity U is simply the force divided by friction coefficient / [Pg.180]

It was shown in Section 6.1 that a component focused at y = 0 by the velocity expression W-U --ay would form a Gaussian zone centered at y- 0. Equation 6.18 shows that the r of the zone is (Dr/a)1/2. In the absence of convection, Drcan be replaced by molecular diffusion coefficient D, yielding [Pg.181]

Although the component zones are Gaussian, plate height expressions are meaningless because the zones (and the resulting separation structure) do not evolve continuously as a result of steady migration. However, resolution and peak capacity are still valid indices of separation, as discussed below. [Pg.181]

To calculate resolution, we need the distance LX between the centers of the two zones of interest as well as mean zone width 4o. The distance LX can be written as [50] [Pg.181]


See other pages where Separation Power of Steady-State Methods is mentioned: [Pg.180]    [Pg.181]    [Pg.183]   


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