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    GC SolutionsSeparation Science GC Solutions is the premier online resource or GC and GC/MS users working across the Asia Pacifc region.

    Covering GC method undamentals, practicalities and troubleshooting it offers chromatographers and analytical chemists a genuine

    e-learning platorm and searchable archive resource.

    www.sepscience.com Issue 8: October 2010

    Tech TipBasis o Interactions in Gas Chromatography,

    Part 1 Non-Polar Interactions

    To ully grasp the concepts o retention and selectivity o GC stationary phases,

    one must frst understand the undamental intermolecular interactions that lead

    to retention. This month we discuss the most dominant o those interactions

    dispersive, non-polar interactions.

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    There are ewer types o intermolecular interactions available orinteractions between solutes and stationary phases in gas chromatographycompared to those possible in liquid chromatography.In addition, themobile phase in GC (the carrier gas) plays no role in adjusting or modiyingthe nature o intermolecular interactions during the run.So, the range opossibilities in retention orces and selectivity is much more limited in GCthan in LC.

    In gas chromatography, molecules can only interact with each other

    through intermolecular orces that all under the umbrella o van derWaals orces.They are listed in Table 1.Van der Waals orces can be overcome or disrupted by thermal motion,

    which increases as temperature increases. This is why liquids evaporateaster when heated. and also why solutes are less retained (elute aster) ingas chromatography as the temperature is raised.

    In gas chromatography, the dominant intermolecular attractive orce isdispersive interactions.Dispersive interactions are known also as temporarydipole interactions, because they result rom transient random distortionsin the electronic clouds o molecules, London forces, ater the scientist whofrst described them.Dispersive interactions exist between all molecules.

    Basis o Interactions in Gas Chromatography,Part 1 Non-Polar InteractionsTo ully grasp the concepts o retention and selectivity o GC stationary phases, one must frst understand the

    undamental intermolecular interactions that lead to retention.This month we discuss the most dominant o thoseinteractions dispersive, non-polar interactions.

    Matthew Klee

    Name Description Molecular traits Characteristic

    Non-Polar

    London2 (1930)

    dispersion

    induced dipole in-

    duced dipole

    All compounds,

    non-polar interaction

    Transient polarization,

    scales with molecular size

    Hydrogen bonding Extreme dipoledipole

    interaction: H acceptor

    interacts with H donor

    Signifcant with

    compounds containing

    OH or -NH groups

    Polar

    Keesom3 (1912) dipoledipole Interaction between

    strong dipoles

    Electronegative groups

    (e.g., halogens, -OR, -NOx,

    -SOx)

    Debye4 (1923) Dipoleinduced dipol e I ntera ct io n between

    a strong dipole and a

    weak dipole

    More polarizable = easier

    induction

    Table 1

    Table 1:Van der Waals1 forces of interactions between molecules.

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    Figure 1

    Figure 1: London dispersive (non-polar) forces dominate the intermolecular interactions in gas

    chromatography.They arise from spontaneous transient distortions, polarization, then coordinatedoscillations in electronic molecular orbitals. The larger the molecule, the larger the dispersive forces, thehigher the strength of interaction, and therefore the higher the retention.

    -

    ---

    --

    +

    +

    +

    +

    +

    +

    -

    -

    -

    -

    --

    +

    +

    +

    +

    +

    +

    Dispersive interactions are non-polar (also called apolar).Dispersiveinteractions arise rom random distortion o the electronic cloud o amolecule, causing a slight electrostatic polarization one side o themolecule becomes more negative, the opposite more positive (Figure 1).

    This spontaneous polarization then induces an opposite polarizationin neighbouring molecules.The opposite charges attract and draw themolecules closer, urther distorting the clouds..A stabilizing oscillationo the charge distortion results within the bulk liquid (in wall coatedopen tubular columns, the stationary phase is considered a liquid). The strength o dispersive interactions track with the size o themolecule; the larger the molecule, the higher its mass, the moreelectrons, the higher the strength o its dispersive orces.Largermolecules have larger electron clouds which are more able to handleelectrostatic distortions.So, the distortions can be o higher magnitudeand o longer duration.For this reason, both boiling points and elutiontemperatures o molecules track with the size o the molecule (Figure 2).

    Although retention in GC is based on the sum o all possibleinteractions, polar + non-polar, some types o molecules such assaturated hydrocarbons (alkanes) can only interact through dispersiveinteractions.Even i a stationary phase were to have polar unctionalgroups and thereore a signifcant possibility or polar interactions,saturated hydrocarbons would only interact with the non-polar,

    dispersive aspect. The basic premise o retention in GC is illustrated in Figure 3.Onecan see in Figure 3 that the solute represented by the blue triangleshas a higher proportion o molecules in the stationary phase than inthe gas phase. As such, it migrates slowly through the column (has ahigh retention time).In contrast, the majority o the solute representedby the green squares is in the gas phase, so it will migrate much asterthrough the column (have a much lower retention time).

    Retention in gas chromatography is an exponential unction otemperature.As temperature is raised, there will be a temperature atwhich the more retained solute (blue triangles) will travel at the same

    The strength of dispersive interactionstrack with the size of the molecule; the largerthe molecule, the higher its mass, the moreelectrons, the higher the strength of its

    dispersive forces.

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    Figure 3

    Figure 3: Inner view o a capillary column. A flm thickness 0.5 m on a 250 m i.d. column represents a

    phase ratio o 125, which is typical o capillary columns. As it is almost impossible to see the

    stationary phase when drawn to scale, the inset shows a representation o the surace magnifed 100

    times to better illustrated solute migration in/out o the phase.The solute with the weaker interactions

    with the stationary phase (green squares) spends more time in the mobile phase and moves aster

    through the column, eluting frst.The compound with stronger interaction with the stationar y phase

    (blue triangles) spends less time in the gas phase and moves slower through the column.

    250mi.d.

    0.50mi.d.

    magnified 100X

    Column wall

    stationary phase

    carrier gas

    column wall

    Figure 2: (A) Retention time trend on-alkanes in a linear temperature programmed capillary GC run. (B)

    Boiling point trend on-alkanes.Retention o in gas chromatography tracks boiling point because o

    dominance o non-polar (dispersive) orces.

    Figure 2

    0

    100

    200

    300

    400

    500

    600

    0 10 20 30 40 50

    Carbon Numbern-Alkane

    Boiling

    Point(oC)

    0

    10

    20

    30

    40

    50

    60

    70

    80

    0 10 20 30 40 50

    Carbon number

    RetentionT

    ime

    A

    B

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    Figure 4

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    1000

    0 25 50 75 100 125 150 175 200 225

    Temperature (oC)

    Reten

    tionFactor(k)

    Figure 5

    1

    10

    100

    1000

    0 50 100 150 200 250 300

    Temperature (oC)

    RetentionFactor(k)

    Solute A

    Solute B

    Solute C

    solute D

    speed as the less retained one in Figure 3 didat the lower temperature.As illustrated inFigure 4, retention decreases approximatelyby or each 23 oC change in temperature.In Figure 5, example trends are plotted on alog scale. One can see that all solutes ollowa similar pattern to a rst approximationbecause the dominant intermolecular orceo interaction is dispersive.There are slightdiferences in slopes or homologs withdiferent unctionalities.These arise rompolar interactions and will be discussed nextmonth.

    References

    1. J. D. van der Waals, The Thermodynamic Theory o Capillarity

    Under the Hypothesis o a Continuous Variation o Density,

    originally published in Dutch in Verhandel. Konink. Akad. Weten.

    Amsterdam, 1, 8, (1893)

    2. Von R. Eisenschitz, F. London, ber das Verhltnis der van der

    Waalsschen Krte zu den Homopolaren Bindungskrten Z.

    Physik, 60, 491-527, (1930)3. W. H. Keesom, On the Deduction o the Equation o State

    From Boltzmanns Entropy Principle, Communications

    Physical Laboratory University o Leiden Supplement, Ed. By H.

    Kamerlingh Onnes, Eduard Ijdo Printer, Leiden, Supplement 24a

    to No. 121-132, 3-2. 0, (1912)

    4. P. J. W. Debye, Die van der Waalsschen Kohsionskrte,

    Physik. Zeitschr., 21, 178-87, (1920)

    Dr Matthew S. Klee is internationally recognizedfor contributions to the theory and practice of gaschromatography. His experience in chemical, pharmaceutical

    and instrument companies spans over 30 years. During thistime, Dr Klees work has focused on elucidation and practicaldemonstration of the many processes involved with GCanalysis, with the ultimate goal of improving the ease of useof GC systems, ruggedness of methods and overall quality ofresults.

    Figure 4: Intermolecular interactions between a solute and a stationary phase lead to retention.

    Retention o solutes is an exponential unction o temperature.Retention decreases by orapproximately every 23 oC change in temperature (solute and stationary phase dependent).

    Figure 5: The exponential retention unction o several solutes plotted on log scale. More volatile solutes(e.g., solute B) will elute earlier and at lower temperatures in a temperature programmed run.To a rstapproximation, or a polar stationary phases the dependence o retention on temperature ollows the

    same trend or all solutes because o dominance o dispersive (non-polar) orces o interaction,

    diferences in slopes arise rom diferences in solute polarities (e.g., solutes A and C). Homologs usuallyhave the the same retention vs temperature slope on a given stationary phase (e.g., solutes B and D).

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    6 . 0 7 . 0 8 . 0 9 . 0 1 0 . 0 1 1 . 0 1 2 . 0 1 3 .0

    1.0

    2.0

    3.0

    4.0

    5.0

    6.0

    7.0

    8.0

    9.0

    10.0( x10,000)

    Fig.2:Top:SIM 1) dataofmasstrace195 relativetoanextractspikedwith17ppt TCAcomparedwithanunspikedextract.

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