LCGC North AmericaMarch 2022

Volume 40

Issue 3

Pages: 111–115

**Choosing a liquid chromatography (LC) column for a particular application can be a surprisingly challenging task. On one hand, column manufacturers give us many options to choose from, including particle types, pore sizes, particle sizes, and different lengths and diameters. On the other hand, we usually don’t have time to experimentally evaluate many combinations of these parameters, and sometimes we end up picking something similar to the columns that are already in the drawer. The “kinetic plot” is a powerful graphical tool that can help leverage the best available theory to help us understand how different combinations of parameters (that is, particle size and length) will perform in terms of the time needed to get to a particular column efficiency (and thus resolution), and therefore make well-informed decisions when choosing columns.**

In the last two installments of “LC Troubleshooting,” we reviewed the basic idea of a “kinetic plot” (1) and how to make the plots from experimental data or data from the literature (2). Ultimately, this graphical tool can be used to make informed decisions when choosing columns and to understand why a column might not be delivering expected performance improvements. This month, we conclude this series of articles by discussing the so-called “Knox-Saleem limit” (KSL), application of kinetic plots to gradient elution conditions, and the impact of extracolumn dispersion on kinetic plots. Finally, we introduce a web-based application that pulls together all of the theory discussed in these installments into a convenient and flexible web-based calculator that allows you to explore the impact of many variables on the kinetic plot on your own.

In last month’s installment, we began discussing the effect of particle size on kinetic plots by showing the kinetic performance limit (KPL) curves for different particle sizes (Figure 1a). Interestingly, these curves cross in the kinetic plot, which means that at any given combination of *t _{0}* and

In Figure 1a, we see that each of the KPL curves touches an oblique asymptote (dashed lines) below which one cannot work regardless of the choice of column length, particle size, and velocity because the pressure drop will exceed the chosen pressure limit.

This oblique asymptote is the KSL and in fact touches the KPLs for different particles sizes at their respective optimal mobile phase velocities (that is, *u _{0,min}*) (3). The point where the KPL and KSL curves touch represents the optimal choice of not only mobile phase velocity and column length, but also of the particle size for each combination of

The KSL can be calculated using equation 1 if the dynamic viscosity of the mobile phase (*η*), the minimum reduced plate height (*h _{min}*), and the

This relationship makes clear that the kinetic performance can be improved by increasing the maximum operating pressure (Δ*P _{max}*; that is, UHPLC vs. HPLC), decreasing the mobile phase viscosity (for example, through the use of high temperatures in LC, or low viscosity eluents in supercritical fluid chromatography [SFC]), reducing the flow resistance (for example, by using monolithic or chip-based columns), or decreasing the minimum reduced plate height (for example, with superficially porous particles, chip-based, or 3D-printed columns) (6). A change in any of these parameters will shift the KSL (and also the KPL curves) to the right, allowing for both faster and more efficient separations. When all other parameters are fixed, doubling Δ

For fundamental comparisons of the separation performance of different column types, it is most practical to use isocratic elution conditions, which is why our discussion of kinetic plots has so far focused on the kinetic plots with *t _{0}* and

- Gradient time should be scaled inversely proportional to the flow rate so that the gradient slope remains constant (10,11).
- If the mobile phase composition is held constant at the beginning of the separation, or at any other point in the elution program, these so-called hold times should also be scaled with the inverse of the flow rate.
- If columns with the same stationary phase chemistry from the same vendor are compared, there is usually little to no difference in selectivity and the same gradient range (initial and final composition) can be used. However, when comparing columns from different vendors, differences in retention may be observed, and it is advisable to tune the initial and final composition of the gradient in such a way that the first and last eluted compounds have similar retention factors (9,11).

As previously mentioned, in the case of gradient elution, the peak capacity (*n _{p}*) is usually the preferred measure of separation performance rather than the column plate count (

The square root dependence in equation 3 is the direct result of the square root dependence of the peak capacity on the column plate number (10). As a result, increasing the column length by a factor of four will only increase the peak capacity by a factor of two. Please note that also in this case the value for Δ*P _{exp}* should include the extracolumn pressure drop as discussed in the next section.

So far in this series, we have not discussed the impact of extracolumn dispersion (ECD) on kinetic plots, which is mathematically convenient. However, peak dispersion outside of the column is often too large to ignore. We discussed the details associated with dispersion in different parts of the LC system in a prior multipart series of articles in this magazine (14–17) and elsewhere (18), and readers interested in these details are referred there. Here, we focus on adjustments that must be made to the kinetic plot calculations to account for both the dispersion that occurs in the LC system outside of the column, and the pressure drop that occurs in different parts of the system.

Corrections to the kinetic plot calculations to account for extracolumn effects can be made using values for the extracolumn dispersion and pressure drop obtained from experiments, or some means of estimation. When it comes to experimental measurements, the column is replaced by a zero dead volume union in order to obtain the extracolumn time (*t _{ec}*) and peak variance (σ

In addition to the effect of the LC system on dispersion of peaks, some of the available operating pressure is also lost because of pressure drops along the connecting tubes, especially when narrow diameter tubes are used. To account for this, the value of Δ*P _{max}* used in calculating the kinetic curves should be reduced by the value of the extra-column pressure drop (Δ

Although no single mathematical step in calculating the kinetic curves is particularly difficult, there are many details to keep track of, and building a calculator correctly from scratch takes some time. Thus, we have built a freely available web-based calculator (www.multidlc.org/kinetic_plot_tool) that incorporates all of the theory discussed in this series of articles, including consideration of extracolumn effects discussed in the previous section. Here, we briefly demonstrate use of the tool by way of an example that shows how it can be used to explore the effects of different variables on the curves, and perhaps develop hypotheses for troubleshooting situations where column performance does not live up to one’s expectations.

Figures 2 and 3 show screenshots of the inputs to the tool. Up to three different conditions can be compared simultaneously. Pre-set configurations for zero, low (~1–2 μL^{2}), and normal (~10–15 μL^{2}) levels of extracolumn dispersion enable quick configuration of the extracolumn inputs; however, each of the system parameters (that is, injector, tubing, and detector) are fully adjustable as well.

Figure 4 shows screenshots of the kinetic plots produced by the tool for two different cases (A and B). In both cases the comparison is between columns packed with fully porous 1.7 μm particles and columns packed with superficially porous 2.7 μm particles. In case A, the tool is configured using the pre-set parameters for a low dispersion system (~1–2 μL^{2}) for both the FPP and SPP columns. Here, we see that the 1.7 μm FPP columns outperform the 2.7 μm SPP ones at the KPL over therange of 5,000 < *N* < 30,000, though the difference is small (*t _{0,FPP}* = 0.28 min vs.

However, when the tool is reconfigured using the preset parameters for a normal dispersion system (~10–15 μL^{2}), we get the curves shown in Figure 4b, where the SPP columns are superior to the FPP ones at the KPL over the entire range of efficiencies shown. On one hand, the superiority of SPP columns is not surprising: manufacturers of sub-2-μm columns have been working to educate users for years about the importance of using these columns in low dispersion systems to maximize their performance potential. On the other hand, this comparison shows the utility of the kinetic plot tool both for making informed choices about column selection, and troubleshooting situations where a column in use does not live up to user expectations.

In this installment of “LC Troubleshooting,” we have continued our discussion of kinetic plots and their utility when selecting column technologies and formats, and troubleshooting columns that appear to not live up to our expectations. The KSL quantifies the best achievable performance (as measured by plate number) in a given analysis time when the particle size is allowed to vary. Kinetic plots can also be used to compare technologies under gradient elution conditions, and when the effects of extracolumn dispersion are accounted for. Finally, we have introduced a freely available web-based kinetic plot tool that leverages all of the theory discussed in this series and enables comparison of up to three different sets of conditions simultaneously. This tool is useful for quickly comparing different column technologies and LC system configurations, and developing troubleshooting hypotheses when things don’t seem to be quite right. It is important to note that all calculations in this series have been done with diffusion coefficients typical of small molecules. When working with large molecules their diffusion coefficients will be very different, and thus the kinetic plots will be very different as well.

(1) K. Broeckhoven and D.R. Stoll, *LCGC N. Am*. **40**(1), 9–12,19 (2022).

(2) K. Broeckhoven and D.R. Stoll, *LCGC N. Am*. **40**(2), 58–62 (2022).

(3) J.H. Knox and M. Saleem, *J. Chromatogr. Sci.* **7**, 614–622 (1969). https://doi.org/10.1093/chromsci/7.10.614.

(4) A.J. Matula and P.W. Carr, *Anal. Chem.* **87**, 6578–6583 (2015). https://doi.org/10.1021/acs.analchem.5b00329.

(5) G. Desmet, D. Cabooter, and K. Broeckhoven, *Anal. Chem*. **87**, 8593– 8602 (2015). https://doi.org/10.1021/ac504473p.

(6) K. Broeckhoven and G. Desmet, *Anal. Chem*. **93**, 257–272 (2021). https://doi.org/10.1021/acs.analchem.0c04466.

(7) Y. Vanderheyden, D. Cabooter, G. Desmet, and K. Broeckhoven, *J. Chromatogr. A.* **1312**, 80–86 (2013). https://doi.org/10.1016/j.chroma.2013.09.009.

(8) X. Wang, D.R. Stoll, P.W. Carr, and P.J. Schoenmakers, *J. Chromatogr. A.* **1125**, 177–181 (2006). https://doi.org/10.1016/j.chroma.2006.05.048.

(9) K. Broeckhoven, D. Cabooter, S. Eeltink, and G. Desmet, *J. Chromatogr. A.* **1228**, 20–30 (2012). https://doi.org/10.1016/j.chroma.2011.08.003.

(10) K. Broeckhoven, D. Cabooter, F. Lynen, P. Sandra, and G. Desmet, *J. Chromatogr. A.* **1217**, 2787–2795 (2010). https://doi.org/10.1016/j.chroma.2010.02.023.

(11) K. Broeckhoven, D. Cabooter, and G. Desmet, *LCGC Europe* **24**, 396–404 (2011).

(12) K. Broeckhoven and G. Desmet, *J. Sep. Sci.* **44**, 323–339 (2021). https://doi.org/10.1002/jssc.202000779.

(13) T.J. Causon, K. Broeckhoven, E.F. Hilder, R.A. Shellie, G. Desmet, and S. Eeltink, *J. Sep. Sci.* **34**, 877–887 (2011). https://doi.org/10.1002/jssc.201000904.

(14) D.R. Stoll, T.J. Lauer, and K. Broeckhoven, *LCGC N. Am*. **39**, 308–314 (2021).

(15) D.R. Stoll and K. Broeckhoven, *LCGC N. Am.* **39**(6), 252–257 (2021).

(16) D.R. Stoll and K. Broeckhoven, *LCGC N. Am*. **39**(5), 208–213 (2021).

(17) D.R.Stoll and K. Broeckhoven, *LCGC N. Am*. **39**(4), 159–166 (2021).

(18) G. Desmet and K. Broeckhoven, *TrAC Trends in Anal. Chem*. **119**, 115619 (2019). https://doi.org/10.1016/j.trac.2019.115619.

Articles in this issue

But Why Doesn’t It Get Better? Kinetic Plots for Liquid Chromatography, Part III: Pulling It All Together

Quick Polar Pesticides (QuPPe): Learning from and Expanding on the Work of Others

Split/Splitless Inlets in Gas Chromatography: What’s Up with All Those Different Glass Inlet Liners?

Charge Detection Mass Spectrometry: What’s the “Big” Deal?

Critical Evaluation of Chromatography Methods: Essential Detective Skills

Enter the Matrix: Improving the Interpretation of Separations Data Using Chemometrics in Analytical Investigations

A Suitable Therapeutic Drug Monitoring Method for Amoxicillin in Plasma by High Performance Liquid Chromatography–UV (HPLC–UV) in Neonates

Related Content