OR WAIT null SECS
Some “LC Troubleshooting” topics never get old because there are some problems that persist in the practice of liquid chromatography (LC), even as instrument technology improves over time. There are many ways for things to go wrong in an LC system that ultimately manifest as deviations from the expected pressure. Developing a short list of the likely causes of these deviations can help streamline our troubleshooting experience when pressure-related problems occur.
Writing this “LC Troubleshooting” column and thinking about topics each month is interesting in the sense that there are some topics that just never get old. Whereas, in the chromatography research world, certain topics or ideas become obsolete as they are displaced by newer and better ideas, in the troubleshooting world there are certain topics that have remained relevant since the very first troubleshooting article appeared in this magazine (LC Magazine at that time) in 1983 (1). Over the last few years, I’ve focused several “LC Troubleshooting” installments on contemporary trends (such as the relatively recent advances in our understanding of the effects of pressure on retention ) in liquid chromatography (LC) that are affecting the way we approach our interpretation of LC results, and approach troubleshooting with modern LC instruments. With this month’s installment, I am starting a series focused on some of the “bread and butter” topics of LC troubleshooting—those elements that are essential for any troubleshooter, no matter the vintage of the system we are working with. The topics at the heart of this series will be highly related to the well-known “LC Troubleshooting” wall chart (3) that hangs in many laboratories. For the first installment in this series, I’ve chosen to focus on problems related to pressure (too low, too high, or fluctuating). I hope LC users young and old will find some useful tips and reminders related to this important topic.
In the area of pressure problems, everything is possible. Sometimes pressure is unexpectedly low, but stable. Other times the pressure is too low, and appears to steadily decrease. The same is true for pressures that are higher than expected. In other cases, the observed pressure may seem to be about right, but it is fluctuating more than usual. Figure 1 illustrates the idea that pressure problems appear in all kinds of different ways, and lists the specific situations that are discussed in this article. The list of pressure-related problems shown in Figure 1 is not exhaustive; in this installment, I focus on those problems that I see most frequently in practice.
A critical step in any troubleshooting exercise —but one that I think is underappreciated— is recognizing that there is a problem to be solved. Recognizing that there is a problem usually amounts to recognizing that what is happening with the instrument is different from what is expected to happen, and our expectations are formed from theories, empirical knowledge, and experience (4).
Before getting into details about what we can expect about pressure, a few words to clarify what it is and how it is measured in LC instruments are warranted. In LC, when we say “pressure,” we are really talking about a “pressure drop” or a “pressure difference.”
These more precise terms are indicated in various equations that relate pressure drop to other variables, such as flow using the symbol ΔP. Most commercially available LC systems have a single pressure readout associated with the pump that reports the pressure drop between the pump and the outlet of the system (the outlet side of a detector flow cell) that, for all practical purposes, is zero, because the atmospheric pressure of about 1 bar is usually small compared to LC operating pressures. This single pressure readout quantifies the total pressure drop across the entire flow path, but does not tell us anything about the pressure drops across individual elements of the flow path (for example, filters, different pieces of connecting tubing, and the column).
Most practical high-performance liquid chromatography (HPLC) is done under conditions where flow through connecting tubing in the system is laminar. Under these conditions, the pressure drops across the different pieces of tubing can be calculated with the accuracy needed for troubleshooting purposes using Poiseulle’s Law:
where ƞ is the dynamic viscosity of the mobile phase, F is the flow rate, and Ltub and dtub are the length and diameter of the tubing, respectively. Calculating the pressure drop using equation 1 is straightforward when all of the values needed are available; however, the dependence of viscosity on mobile-phase composition and temperature is a bit complex. Fortunately, there are some freely available web-based tools that take these factors into account (for example, see reference , and https://www.multidlc.org/dispersion_calculator), and provide users with quick estimates of the expected pressure drops for the tubes in their systems.
The pressure drop across the LC column itself (assuming the column is packed with particles) can be calculated using equation 2 (or similar). Like equation 1 for open tubes, the pressure drop depends on the column length, mobile-phase viscosity, and the flow rate (through the interstitial mobile phase velocity, ue). Different in equation 2 are the Φ term that quantifies the permeability of the packed particle bed, and the particle size term, dp2.
As with equation 1, calculating the pressure drop across the column is straightforward once all of the values for length, viscosity, and other variables are in hand, but they are not all easy to come by. Once again, there are freely available simulators that can calculate the pressure drop for conditions of interest. Two such simulators that I am familiar with are the web-based LC simulator maintained by my group (https://www.multidlc.org/hplcsim), and the spreadsheet-based simulator developed more recently by Prof. Davy Guillarme’s group (see ; https://ispso.unige.ch/labs/ fanal/practical_hplc_simulator:en).
The other elements of an LC flow path that can contribute substantially to the pressure drop measured at the pump are inline filters (and guard columns, though these can be treated like columns as above). Most inline filters sold for use in analytical LC systems are designed in a way that they will not contribute more than a few bar to the total pressure drop under typical conditions (that is, less than 5 mL/min). When debris begins to accumulate on the filter, the pressure drop across the filter will increase, and become highly, and sometimes non-linearly, dependent on operating conditions (for example, flow rate and mobile-phase composition). Because it is difficult to cope with this hard-to-predict behavior, in my laboratory we simply change the filter if the pressure drop across it exceeds about 10 bar.
Throughout the hundreds of “LC Troubleshooting” articles John Dolan wrote, he emphasized the value of “rules of thumb” in effective troubleshooting (7). I completely agree, and think the value of these ideas—which are informed both by theory and experience—cannot be overstated. As an example of a rule of thumb that is useful in the context of troubleshooting pressure problems, the one that we use in my group is that the pressure drop across all of the tubing (no column) in a “typical” LC system is about 30 bar under the following conditions (if the observed pressure is much lower or higher than that, this should trigger a thought that something is not right):
There are two main problems that lead to pressures that are lower than expected.
Most problems involving higher than expected pressure are somehow related to accumulation of debris somewhere in the system. The origins of this debris vary; it can come from particulate matter in the injected sample, molecules that are soluble in the sample solvent but precipitate it the mobile-phase stream, polymeric material shed by pump and injector seals, and so on. The specific nature of the problem that results from this debris depends strongly on how the system is configured. Determining where the obstruction is in the system can be tricky. A systematic approach to finding out where the problem lies involves removing components from the flow path one at a time, start- ing from the downstream end. For example, suppose we are running at 1 mL/min, and we observe a pressure at the pump of 600 bar, which is high compared to a normal operating pressure of 250 bar. With the flow off, remove the detector from the flow path. Turn the pump back on and record the pressure. If it has only decreased by 5 bar to 595 bar, then we know that the obstruction does not lie in the detector flow path. Again, with the flow off, remove the tubing between the detector and the column outlet. Turn the flow back on and record the pressure. If it has decreased another 10 bar to 585 bar, then we know that the tubing between the column outlet and the detector is not the source of the problem. Next, remove the column, turn the flow back on, and record the pressure. There should be a significant difference between the pressure recorded with and without the column connected. Suppose in this case that the pressure is still 365 bar even without the column connected, which would be abnormal in any typical analytical LC system. Next, suppose that upon removing the inline filter installed immediately upstream from the column the pressure drops to 20 bar. This would tell us that the pressure drop over the filter itself was 345 bar (far higher than expected), indicating that the filter should be thrown away and replaced. This “one-piece-at-a-time” approach can feel tedious when trying to get an instrument back on track, but it is the most reliable way to isolate the problem. The three most commonly encountered scenarios are:
Most modern LC pumps are based on some variation of a reciprocating dual piston design, where the pressure variation that occurs at the end of each piston stroke can be minimized, but is difficult to eliminate entirely. The specification for modern pumps is that the pressure variation should not exceed about 1%. If the observed variation is much larger than 1%, then it is most likely because of one of two reasons.
In this first installment on essential topics in LC troubleshooting, I have discussed situations where the observed system pressure is somehow different from what is expected or normal. Effective troubleshooting for this type of problem begins with a sense for what the expected system behavior is, so that a deviation from those expectations is noticeable. While there a many different potential causes of pressure related problems (too low, too high, or fluctuation), most problems can be connected to five or six specific causes. Understanding this short list of likely causes provides a good place to start troubleshooting, but does not capture all possibilities. Readers interested in learning about a deeper list of causes and solutions are referred to the “LCGC Troubleshooting” wallchart (3).
(1) D. Runser, LC Magazine 1(1), 10–16 (1983).
(2) T. Kempen and D.R. Stoll, LCGC North Am. 39(10), 471–475 (2021).
(4) D.R. Stoll, LCGC North Am. 38(10), 544–547 (2020).
(5) D.R. Stoll and K. Broeckhoven, LCGC North Am. 39(6), 252–257 (2021).
(6) D. Guillarme, B. Bobaly, and J.-L. Veuthey, LCGC North Am. 39(3), 144–145 (2021).
(7) J. Dolan, LCGC North Am. 32(8), 546–551 (2014).