UHPLC TIP: Reducing the Column Temperature to Offset Frictional Heating Effects (Causing Poor Resolution)

HPLC column temperature is a critical variable that we adjust and optimize during method development. We use it as a variable during the method development process to improve solubility, optimize peak shape and increase resolution. Once established, it must be carefully controlled during the method analysis to provide reliable and reproducible analysis results. Change the column temperature and you may also change the results obtained. This is a fundamental method development tool and must not be forgotten.

If you are developing a new UHPLC method OR perhaps scaling an HPLC method to utilize 2.5 micron or smaller support particles, then you may observe a loss of resolution or poor peak shape in the new method. There are many reasons why this may occur, and the most common ones relate to not optimizing all of the method parameters correctly when scaling the method (e.g. dwell volume too large, flow cell volume too large, injection volume too large, sample rate too slow, flow rate not optimized, mobile phase composition changes not in scale with the gradient...). But there is another reason...

Resolution may be reduced or lost when all of the initial scaling and instrument set-up parameters are optimized. What is the most likely reason for this? In many cases the use of substantially higher flow rates (relative to linear flow rates) and the use of smaller diameter particles results in much higher backpressures (you may recall that if you halve the particle size, the backpressure increases 4x). The resulting backpressure might be 2, 3 or even 4 times higher than observed in the original method. While these higher backpressures were well within the operating parameters of the HPLC system used, the results obtained were poor. The possible cause? The much higher backpressure increased the amount of frictional heating inside the column, raising the actual analysis method temperature and changing the separation conditions. 

Pushing mobile phase (liquid) through a chromatography column generates heat and pressure. The heat generated increases the actual temperature of the column and reduces the viscosity of the fluid. In conventional columns (i.e. 4.6 x 150 mm, 5u) at 1.00 ml/min, this heating effect is minimal, but at much greater column pressures, > 400 bars, the frictional effects may be substantial. These types of very high pressures may be seen with methods which utilize columns containing the smallest particles (1.9 to 2.5 micron). Enough to change the temperature in the column by several degrees (e.g. >5 degrees C) and result in different method conditions. So, what can you do about this? The most direct way to address the problem is to run the same method at a lower temperature (perhaps decrease by 5 C to start with). This will slightly raise the backpressure (lower temperature equals higher viscosity), but it should cool the column and restore the original temperature conditions used. Additionally, we suggest that you always start column equilibration using a flow ramp to gradually increase the flow over time and reduce the overall heating effect and resulting "shock" placed on the column. An initial delay at equilibration may help reduce these effects (gradually ramp up to the regular flow rate and hold). You may need to try several temperatures and this may be easiest to do if your HPLC has a column compartment with heating and COOLING capabilities. Optimizing the temperature and internal pressures may increase the column lifetime and result in better overall data reproducibility.

Ion Exchange Resin Mesh Size Number to Millimeter (mm) Conversion Table

Chromatography Ion Exchange Resins are often sold based on Mesh Size Number. Here is a table showing the conversion to particle size in microns or millimeters.

Mesh Size / Number	Particle Size (mm)
1250	0.010
625	0.020
550	0.025
400	0.037
325	0.044
270	0.053
230	0.063
200	0.075
170	0.090
140	0.106
120	0.125
100	0.150
80	0.180
70	0.212
60	0.250
50	0.300
45	0.355
40	0.425
35	0.500
30	0.600
25	0.710
20	0.850
18	1.000
16	1.180
14	1.400
12	1.700
10	2.000
8	2.360
6	3.350
4	4.750

Pressure Drop Across an HPLC / UHPLC Column

Many of you prefer tables of data over equations that you must work out. So, instead of providing you with another equation, I have done some basic measurements for you to provide a general overview of how particle size (porous) effects System backpressure.

For simplicity, let us start with a few parameters. Pore Volume = 0.70; Linear Velocity = 1.44 mm/sec; Solvent Viscosity = 0.89 cP at 25C (Water). 

Pore Volume and Flow Resistivity will vary by column type. Obviously the back pressure will be higher with more viscous solvents (e.g. EtOH is 1.20 cP) and lower with less viscous solvents (e.g. ACN is 0.34cP). A Table of HPLC Solvent Viscosity values can be found here [ http://www.hplctools.com/lcsolvent.htm ]. Linear flow rates have been used for all column I.D.'s to better illustrate the relationship between column dimensions and flow rate. If you double the flow rate, then the pressure will approximately double as well. 

Note that when run at traditional linear velocities, most 2.5u particles are within the maximum pressure limits of most HPLC systems (under 400 bars). Only the newer sub 2.0 micron particles used in long columns exceed the 400 bar limit. The higher maximum pressure limits of many UHPLC systems allow the use of higher flow rates with these particles. Naturally, you should optimize both column efficiency and system dwell volume when developing any UHPLC method. Failure to optimize the dwell volume (and minimize all volumes) may result in very poor chromatography separations. Meeting any/all backpressure requirements to run a method does not translate to success in sample analysis. Successful ultra-fast separations require ultra-low system dwell volumes, higher sampling rates and usually smaller flow cell volumes.

HPLC Column I.D. (mm)	Particle Size (u)	Column Length (mm)	Flow Rate (mL/min)	Observed System Back Pressure (Bars)
4.6	5	250	1.000	89
4.6	5	150	1.000	54
4.6	5	100	1.000	36
4.6	5	50	1.000	18
4.6	3.5	250	1.000	182
4.6	3.5	150	1.000	109
4.6	3.5	100	1.000	73
4.6	3.5	50	1.000	36
4.6	2.5	250	1.000	357
4.6	2.5	150	1.000	214
4.6	2.5	100	1.000	143
4.6	2.5	50	1.000	71
4.6	1.9	250	1.000	618
4.6	1.9	150	1.000	371
4.6	1.9	100	1.000	247
4.6	1.9	50	1.000	124
3.0	5	250	0.430	90
3.0	5	150	0.430	54
3.0	5	100	0.430	36
3.0	5	50	0.430	18
3.0	3.5	250	0.430	184
3.0	3.5	150	0.430	110
3.0	3.5	100	0.430	74
3.0	3.5	50	0.430	37
3.0	2.5	250	0.430	361
3.0	2.5	150	0.430	217
3.0	2.5	100	0.430	144
3.0	2.5	50	0.430	72
3.0	1.9	250	0.430	625
3.0	1.9	150	0.430	375
3.0	1.9	100	0.430	250
3.0	1.9	50	0.430	125
2.1	5	250	0.210	90
2.1	5	150	0.210	54
2.1	5	100	0.210	36
2.1	5	50	0.210	18
2.1	3.5	250	0.210	184
2.1	3.5	150	0.210	110
2.1	3.5	100	0.210	73
2.1	3.5	50	0.210	37
2.1	2.5	250	0.210	360
2.1	2.5	150	0.210	216
2.1	2.5	100	0.210	144
2.1	2.5	50	0.210	72
2.1	1.9	250	0.210	623
2.1	1.9	150	0.210	374
2.1	1.9	100	0.210	249
2.1	1.9	50	0.210	125

* The results obtained in this table from are from one of our HPLC systems and reflects the total system backpressure (what the pressure gauge reads), with the column inline. Your results may vary due to differences in HPLC system used, flow path, tubing ID, column choice and mobile phase selected.