Gas-Liquid Chromatography
Fig.1 shows a scheme of the
home-made GLC-apparatus which can be used for "classical" as well as for
"non-steady-state" gas-liquid chromatography <1, 2>. The calculation of g¥ from the obtained data and some typical g¥-values can be seen in Fig. 2 and 3.

Fig. 1: Scheme of the gas-liquid
chromatograph applicable
in the "classical" and
the "non-steady-state" mode
Fig. 2:
Evaluation of chromatographic data
More
Information about the data evaluation
Fig. 3:
Typical g¥-results
The GLC technique requires the
careful preparation of the column and allows the measurement of a great number of g¥
in a rather short time. The amount of solvent in the column has been determined
gravimetrically. In order to check if solvent losses occur during the measurements, the
liquid loading is determined before and after the measurement. This is taken into account
assuming linear solvent loss during the isothermal measurements. With the use of
presaturators the loss of solvent can be kept to a minimum. Furthermore the experimental
conditions (gas flow, solvent loss, ...) were checked by measuring the retention time of a
reference substance in regular intervals.
Dilutor Method
The experimental setup for the
dilutor method is shown schematically in Fig. 4. and Fig. 5

Fig. 4:
Scheme of the dilutor
picture of the device


Fig. 5: Scheme of the equilibrium cell
With a constant inert gas flow a highly diluted component (solute) is stripped from a
liquid solution (solvent). The variation of solute concentration in the gaseous phase is
measured with the help of a gas chromatograph <3>. In Fig. 6 values for g¥ are obtained from the graph t vs. ln peak area (concentration of
the solute in the vapor phase).

Fig. 6 Evaluation of data
from the dilutor method
A detailed
description of the measurement procedure and the data analysis can be found by Leroi et
al. (1977) and Duhem and Vidal (1978). The real behavior of the gas phase is taken into
account with the help of fugacity coefficient of the solute in the saturated state. The
values are calculated with the help of the second virial coefficient. For the vapor
pressure calculation (Antoine, Wagner, DIPPR, ...) the equation with the
smallest deviations to experimental vapor pressure data stored in the Dortmund Data
Bank is used.
References
Schiller, M.; Gmehling, J.
Measurement of Activity Coefficients at Infinite Dilution Using Gas-Liquid Chromatography.
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Eng. Data, 1992, 37, 503-508.
Dallinga, L.; Schiller, M.; Gmehling,
J. Measurement of Activity Coefficients at Infinite Dilution Using Differential
Ebulliometry and Non-Steady-State Gas-Liquid Chromatography. J. Chem. Eng. Data 1993,
38, 147-155.
Leroi, J.-C.; Masson, J.-C.; Renon, H.; Fabries, J.-C.; Sannier, H. Accurate Measurement
of Activity Coefficients at Infinite Dilution by Inert Gas Stripping and Gas
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Gmehling, J.; Kolbe, B. Thermodynamik, 2nd ed.; VCH-Verlag: Weinheim, 1992.
Gmehling, J.; Menke, J.; Schiller, M. Activity Coefficients at Infinite Dilution,
DECHEMA Chemistry Data Series IX, DECHEMA: Frankfurt, 1994; Parts 1-4.
Gruber, D.; Langenheim, D.; Moollan, W.C.; Gmehling, J. Measurement of Activity
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Gruber, D.; Langenheim, D.; Moollan, W.C.; Gmehling, J. Measurement of Activity
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Solutes with N-Methyl-2-piperidone as Stationary Phase. J. Chem. Eng. Data, 1998a,
43, 226-229.
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Electron. J. Phys.-Chem. Data, 1998b, 3, 215-224.
D. Gruber, M. Topphoff, J. Gmehling; Measurement of
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Various Solutes with the Stationary Phases 2-Pyrrolidone and N-Methylformamide; J. Chem.
Eng. Data 43, 935-940 (1998)
D. Gruber, M. Krummen, J. Gmehling; Bestimmung von
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Ing.- Tech. 71, 503-508 (1999).
