Nitrogen cannot be used as carrier gas for GC. How sure are you about that? In this presentation we tackle what we call the “van Deemter indoctrination”. Take a look at our recent accomplishments and convince yourself to give it at try. Particularly now when more and more laboratories are suffering from inconsistent supplies of helium.
16. That’s because we all suffer from
the “van Deemter indoctrination”
Don’t worry, I’ve been a victim myself too…
17. Take a look at our experiences
and try to cure yourself too!
18. J. J. van Deemter was a briljant Dutch physicist.
He worked for the Royal Dutch Shell laboratory
In Amsterdam (The Netherlands) in the 1950s.
He was employed as chemical engineer and only
had little direct interest in chromatography.
19. In those days, the mathematical description of
the chromatography process was rather complex.
20. In those days, the mathematical description of
the chromatography process was rather complex.
This was mainly due to improper modelling.
21. However, after much experimentation and plotting,
a very simple equation could be derived.
van Deemter J. J., Zuiderweg F. J. & Klinkenberg A.
“Longitudinal diffusion and resistance to mass transfer as causes of nonideality in chromatography.”
Chem. Eng. Sci. 5:271-89, 1956.
22. This equation, which is known as the van Deemter
equation, was the first to describe the chromato-
graphic process correctly.
23. H = A + B/u + Cu
H = height of one theoretical plate, cm
u = average linear velocity, cm/s
24. H = A + B/u + Cu
In order to work under optimal conditions,
plate height H has to be minimal.
25. THE A TERM = EDDY DIFFUSION
Peak broadening due to path lenghts differences in packed
GC columns. A = 0 for capillary columns.
26. THE A TERM = EDDY DIFFUSION
Peak broadening due to path lenghts differences in packed
GC columns. A = 0 for capillary columns.
27. THE A TERM = EDDY DIFFUSION
Peak broadening due to path lenghts differences in packed
GC columns. A = 0 for capillary columns.
28. THE A TERM = EDDY DIFFUSION
Peak broadening due to path lenghts differences in packed
GC columns. A = 0 for capillary columns.
29. THE A TERM = EDDY DIFFUSION
Peak broadening due to path lenghts differences in packed
GC columns. A = 0 for capillary columns.
30. THE B TERM = LONGITUDINAL DIFFUSION
Peak broadening due to multidirectional diffusion.
Indirectly proportional to flowrate.
31. THE B TERM = LONGITUDINAL DIFFUSION
Peak broadening due to multidirectional diffusion.
Indirectly proportional to flowrate.
32. THE B TERM = LONGITUDINAL DIFFUSION
Peak broadening due to multidirectional diffusion.
Indirectly proportional to flowrate.
33. THE B TERM = LONGITUDINAL DIFFUSION
Peak broadening due to multidirectional diffusion.
Indirectly proportional to flowrate.
34. THE C TERM = RESISTANCE TO MASS TRANSFER
Peak broadening due to equilibrium kinetics in mobile and
stationary phase. Directly proportional to flowrate!
flowrate!
Stationary phase
35. THE C TERM = RESISTANCE TO MASS TRANSFER
Peak broadening due to equilibrium kinetics in mobile and
stationary phase. Directly proportional to flowrate!
flowrate!
Stationary phase
36. THE C TERM = RESISTANCE TO MASS TRANSFER
Peak broadening due to equilibrium kinetics in mobile and
stationary phase. Directly proportional to flowrate!
flowrate!
Stationary phase
37. THE C TERM = RESISTANCE TO MASS TRANSFER
Peak broadening due to equilibrium kinetics in mobile and
stationary phase. Directly proportional to flowrate!
flowrate!
Stationary phase
38. Both B and C terms react opposite to flowrate
changes.
39. Both B and C terms react opposite to flowrate
changes.
There is an optimal flow!
40. This is how a typical van Deemter curve looks like.
3,5
3
2,5
2
H, cm
1,5
1
0,5
0
0 0,5 1 1,5 2 2,5
Flow rate, mL/min
41. And this is the optimal flow region.
3,5
3 Optimal flow region
2,5
2
H, cm
1,5
1
0,5
0
0 0,5 1 1,5 2 2,5
Flow rate, mL/min
42. Key variables that determine curve shape and optimal
flow region are column ID and carrier gas type.
43. Key variables that determine curve shape and optimal
flow region are column ID and carrier gas type.
44. Key variables that determine curve shape and optimal
flow region are column ID and carrier gas type.
45. Influence of carrier gas type.
3,0
Nitrogen
2,5
2,0
H, cm
1,5
Helium
1,0 Hydrogen
0,5
0,0
0 0,5 1 1,5 2 2,5
Flow rate, mL/min
46. Experimental details.
3,0
Test compound: 2-ethyl hexanoic acid Nitrogen
2,5 Column: 20 m x 0.18 mm I.D. x 0.18 µm df
Phase: Rxi-5 Sil MS
Manufacturer: Restek (# 43602)
2,0
H, cm
1,5
Helium
1,0 Hydrogen
0,5
0,0
0 0,5 1 1,5 2 2,5
Flow rate, mL/min
50. Van Deemter tells us: “hydrogen is best”.
We advise to use hydrogen for fast(er) GC
applications. In combination with MS you have to
cope with a loss in sensitivity and a risk of activity.
52. Approach when keeping the same column:
Divide the isothermal stages of your oven program
by two and double all the programming rates (head
pressure stays the same).
53. Approach when keeping the same column:
Divide the isothermal stages of your oven program
by two and double all the programming rates (head
pressure stays the same).
Thus:
30C (2 min) to 250C at 10C/min (Helium)
=
30C (1 min) to 250C at 20C/min (Hydrogen)
68. But beware,
It’s a struggle to convice company safety officers.
You need to invest in sensors.
69. But beware,
It’s a struggle to convice company safety officers.
You need to invest in sensors.
You need to invest in generators.
70. But beware,
It’s a struggle to convice company safety officers.
You need to invest in sensors.
You need to invest in generators.
And sometimes it simply does not work!
88. Approach when keeping the same column:
Just leave everything as it is
(including head pressure)!
89. Approach when keeping the same column:
Just leave everything as it is
(including head pressure)!
Thus:
30C (2 min) to 250C at 10C/min (Helium)
=
30C (2 min) to 250C at 10C/min (Nitrogen)
110. More information?
Dr. Joeri Vercammen
IS-
Managing Expert IS-X
www.is-x.be
j.vercammen@is-x.be
http://www.linkedin.com/in/joerivercammen
Also check out our other presentations!
111. Acknowledgements:
C. De Weerdt
E. Van Brussel
A. De Caluwé
R. Heus
P. Ryckaert
M. Van Lancker