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 diffusio
On the statistical independence of various column contributions to band broadening. Part 3: Independent treatment of longitudinal diffusion in the plate model
โ Scribed by Nilsson, Olle
- Publisher
- John Wiley and Sons
- Year
- 1982
- Tongue
- English
- Weight
- 755 KB
- Volume
- 5
- Category
- Article
- ISSN
- 0935-6304
No coin nor oath required. For personal study only.
โฆ Synopsis
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 classical experimental HETP value, H = L/jitheor, and the underlying true theoretical plate height, AL, is found to be
when (u'p is the total column contribution to band broadening,L isthecolumnlength,& istheaveragediffusioncoefficient ofthe sample component in the mobile phase, 4 is its value in the stationary phase, and ii is the average linear velocity of the mobile phase. The mobile phase displacement, as well as the mass exchange process, is assumed to be continuous, but the application of the plate concept conditions leads to a mass balance equation that can be interpreted as belonging to a modified discontinuous plate model. The contributions 2&,/0 and k 2 &/ii from longitudinal sample diffusion in the mobile and stationary phases, respectively, are consistent with the assumption that the processes are statistically independent, although the common solution technique of the differential equations does not take full account of this independence.
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