Chromatographic theory

10 Chromatographic theory





Void volume and capacity factor


Figure 10.1 shows an HPLC column packed with a solid stationary phase with a liquid mobile phase flowing through it.



If a compound does not partition appreciably into the stationary phase, it will travel through the column at the same rate as the solvent. The length of time it takes an unretarded molecule to flow through the column is determined by the void volume of the column (Vo). The porous space within a silica gel packing is usually about 0.7 × the volume of the packing; a typical packing volume in a 0.46 × 15 cm column is ca 2.5 cm3. Thus, in theory, it should take solvent or unretarded molecules, flowing at a rate of 1 ml/min, ca 1.8 min to pass through the void volume of such a column (the internal space is likely to be reduced where the silica gel has been surface coated with stationary phase). The length of time it takes a retarded compound to pass through the column depends on its capacity factor (K′), which is a measure of the degree to which it partitions (adsorbs) into the stationary phase from the mobile phase:



image



where Vo is the void volume of the column; Vr is the retention volume of the analyte; to is the time taken for an unretained molecule to pass through the void volume; and tr is the time taken for the analyte to pass through the column. In the example shown in Figure 10.1, compound B has a larger capacity factor than compound A. For example, if a compound had a K′ of 4, the Vo of a column was 1 ml and the solvent was flowing through the column at 1 ml/min, the total time taken for the compound to pass through the column would be 5 min, i.e. for the 1 min required to pass through the void space in the column 4 min would be spent in the stationary phase. This is a simplification of the actual process but it provides a readily understandable model. As can be seen in Figure 10.1 the peaks produced by chromatographic separation actually have width as well as a retention time and the processes which give rise to this width will be considered later.





Origins of band broadening in HPLC



Van Deemter equation in liquid chromatography


Chromatographic peaks have width and this means that molecules of a single compound, despite having the same capacity factor, take different lengths of time to travel through the column. The longer an analyte takes to travel through a column, the more the individual molecules making up the sample spread out and the broader the band becomes. The more rapidly a peak broadens the less efficient the column. Detailed mathematical modelling of the processes leading to band broadening is very complex.1 The treatment below gives a basic introduction to the origins of band broadening. The causes of band broadening can be formalised in the Van Deemter equation (Equation 3) as applied to liquid chromatography:



image     Equation 3



H is the measure of the efficiency of the column (discussed above); the smaller the term the more efficient the column.


u is the linear velocity of the mobile phase, simply how many cm/s an unretained molecule travels through the column, and A is the ‘eddy’ diffusion term; broadening occurs because some molecules take longer erratic paths while some, for instance those travelling close to the walls of the column, take more direct paths, thus eluting first. As shown in Figure 10.3, for two molecules of the same compound, molecule X elutes before molecule Y. In liquid chromatography the eddy diffusion term also contains a contribution from streaming within the solvent volume itself, i.e. A (see the Cm term) is reduced if the diffusion coefficient of the molecule within the mobile phase is low because molecules take less erratic paths through not being able to diffuse out of the mainstream so easily.



B is the rate of diffusion of the molecule in the liquid phase, which contributes to peak broadening through diffusion either with or against the flow of mobile phase; the contribution of this term is very small in liquid chromatography. Its contribution to band broadening decreases as flow rate increases and it only becomes significant at very low flow rates.


Cs is the resistance to mass transfer of a molecule in the stationary phase and is dependent on its diffusion coefficient in the stationary phase and upon the thickness of the stationary phase coated onto silica gel:



image



where d2 thickness is the square of the stationary-phase film thickness and Ds is the diffusion coefficient of the analyte in the stationary phase.


Obviously the thinner and more uniform the stationary-phase coating, the smaller the contribution to band broadening from this term. In the example shown in Figure 10.4, molecule Y is retarded more than molecule X. It could be argued that this effect evens out throughout the length of the column, but in practice the number of random partitionings during the time required for elution is not sufficient to eliminate it. As might be expected, Cs makes less contribution as u decreases.


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Jun 24, 2016 | Posted by in PHARMACY | Comments Off on Chromatographic theory

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