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. Author manuscript; available in PMC: 2013 Feb 4.
Published in final edited form as: J Fluid Mech. 2012 Mar 9;697:436–454. doi: 10.1017/jfm.2012.76

Figure 3.

Figure 3

The number of theoretical plates N = L22 as a function of dimensionless electro-osmotic velocity u* = ueo/v0 for three different detector to injection point distances (L) and a range of sample loading characterized by the Péclet number P = v0Γ/D. Here N0 is the “ideal” value of N in the absence of electromigration dispersion.