It is shown theorectically that the classical formula for calculating the theoretical plate number from squared first central moment, fkg, and second central moment, u2, according to fitheor = f&du2, is valid only when the capacity ratio, E, approaches infinity. The general relation between the clas
On the statistical independence of various column contributions to band broadening. Part 1: Second moment contributions from statistically independent, longitudinal diffusion in both phases
โ Scribed by Nilsson, Olle
- Publisher
- John Wiley and Sons
- Year
- 1982
- Tongue
- English
- Weight
- 615 KB
- Volume
- 5
- Category
- Article
- ISSN
- 0935-6304
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โฆ Synopsis
The total length-based second moment contribution from longitudinal sample diffusion in both phases on a column, o$,, is derived by adding individual partial differential contributions to a partial differential equation accounting for the longitudinal diffusion processes only. Although each diffusion-dispersed sample part is equilibrated between two phases, the resulting o&, (= 2k,f, + 2Rf,) can be interpreted as the sum of two independent contributions in accordance with the variance addition rule. (6, and 6, are the mean diffusion coefficients and f,and f, the mean residence times of the sample in the mobile and stationary phases, respectively.) The same expression is derived from the random walk model of Giddings by treating the diffusional process in each phase as statistically independent of the other processes. Under these conditions the broadening contribution from longitudinal diffusion in themobile phase is shown to be independent of the velocity profile.
๐ SIMILAR VOLUMES
The mass balance changes of Said's so-called "stage" model, based on the movement of the mobile phase with mean velocity ! (=L/i,), are synchronized by introduction of the relaxation timeof Giddings, t, = 1 /(km+ k,) where kmand ksare thegeneral overall mass rate constants for sample transfer to and