DOI:
10.1039/A908654D
(Communication)
Analyst, 2000,
125, 21-24
Trace level analysis of VOCs and semi-VOCs in aqueous
solution using a direct insertion membrane probe and trap and release
membrane introduction mass spectrometry
Received 1st November 1999, Accepted 30th November 1999
First published on UnassignedUnassigned26th January 2000
Abstract
A new design for a trap and release membrane introduction mass
spectrometry (T&R-MIMS) system using a removable direct insertion
membrane probe (DIMP) for combined trace level analysis (low or sub ppb
range) of volatile (VOC) and semi-volatile organic compounds (SVOCs) is
reported. The system differs from the original T&R-MIMS system (M. Leth
and F. R. Lauritsen, Rapid Commun. Mass Spectrom., 1995, 9, 591)
as it uses a removable DIMP probe to place a capillary membrane loop inside
the ion source block exactly between two parallel filaments. The more
versatile DIMP-T&R-MIMS system can be operated, during the trapping
step of T&R-MIMS analysis, in the standard MIMS mode for VOC detection;
during the T&R-MIMS thermal desorption step needed for SVOC analysis,
the system permits faster and more uniform heating of the membrane, thus
SVOC sensitivity is improved and memory effects are minimized.
Introduction
Membrane introduction mass spectrometry (MIMS)1 is a recent,
fast-growing technique for the analysis of volatile organic compounds
(VOCs), especially in aqueous matrixes. From chemical to biochemical and on
to physiological monitoring, MIMS has found widespread use; its many
advantages include simplicity, speed, high sensitivity, precision, nearly
real-time and in situ monitoring.1MIMS benefits from selective transport of VOCs through a hydrophobic
membrane, often of silicone polymer; VOCs are transferred frequently
without any extraction or pretreatment from the aqueous matrix directly
into a mass spectrometer. The membrane also works as an efficient interface
between the matrix and the high vacuum of the mass spectrometer. The VOCs
migrate from the aqueous solution to the membrane, concentrate in and
diffuse through the membrane, and evaporate from the membrane surface
directly into the high vacuum ion source region of a mass spectrometer, in
which they are ionized and detected normally at trace levels (low ppbs or
less).1
For the analysis of semi-volatile organic compounds (SVOCs) and polar
VOCs in aqueous matrixes, standard MIMS has been, however, unsatisfactory
since the detection limits are often too high to be useful. Several
approaches have therefore been proposed to improve MIMS detection limits
for SVOCs and concurrently to lower the detection limits for VOCs: a
typical approach has been to combine MIMS with a preconcentration
(trapping) method, using solid adsorbents,2
cryotrapping,3 purging,4 headspace trapping,5 or analyte ion trapping.6 Ultrathin composite membranes (25–0.5
μm)7 normally reinforced with a
microporous support have also been used to reduce transport time through
the membrane. Since the analyte permeability is inversely dependent on
membrane thickness, the ultrathin membranes alleviate the effect of low
diffusivity or low solubility (or both) of SVOCs in silicone. Chemical
derivatization of the SVOCs8 or indirect
monitoring of a related VOC analyte can also be useful alternatives for
trace SVOC analysis by MIMS; recently, for instance, the selective and
sensitive quantitation of cyanogenic glycosides in cassava root extracts
was performed via hydrolysis and MIMS monitoring of the released
ketone.9
But so far the most generally applicable approach for trace SVOC
analysis by MIMS has been offered by the trap and release MIMS
(T&R-MIMS) technique developed by Leth and Lauritsen and
co-workers10 and Matz and Lennemann.11 Poor responses for SVOCs with standard MIMS
often result from their inefficient evaporation from the membrane to the
gas phase. The original fully-integrated T&R-MIMS system10 is unique since it uses no external trapping:
the SVOCs are preconcentrated inside the membrane itself, before fast
thermal desorption12 promotes efficient
transport of the SVOCs into the gas phase. A tubular membrane, mounted
between two 1/16 in stainless-steel tubes, passes straight through the ion
source, and a long slit parallel to both the membrane and the filament
allows heat radiation from the filament to reach the membrane continuously.
An aqueous solution of the SVOCs (at near 0 °C or room temperature
since the SVOC’s solubility in the silicone membrane normally
decrease with temperature) is flushed typically for 20 min through the
membrane inlet, and during this period the SVOCs dissolve in, diffuse
through and concentrate inside the membrane. The cooling fluid is then
removed by pumping through the lines a plug of air for typically 50
s;10b when the air plug reaches
the membrane, the radiant heat from the filament rapidly heats the membrane
to more than 300 °C. As a result, the SVOCs dissolved in the membrane
evaporate rapidly, and are efficiently transferred to the gas phase. When
compared to standard MIMS, responses are improved, typically 50 or more
times higher; hence lower detection limits on the low or sub ppb range are
obtained.
We now report on a more versatile and advantageous design for a trap and
release MIMS system that uses a removable direct insertion membrane probe
(DIMP)13 to place a capillary membrane loop
inside the ion source block exactly between two parallel filaments. The
new, more versatile DIMP-T&R-MIMS system allows combined trace level
analysis (low or sub ppb range) of both volatile (VOC) and semi-volatile
organic compounds (SVOCs); it promotes, during the thermal desorption step
needed for SVOC analysis, uniform and fast membrane heating and efficient
ionization. Hence, sensitivity is enhanced and memory effects are
reduced.
Experimental
MS detection (scan speed of typically 6 spectra min−1)
was performed using 70 eV electron ionization and an Extrel (Pittsburgh,
PA) mass spectrometer fitted with a high transmission (3/4 in) quadrupole.
The standard ion source was used with just a minor modification: the id of
one of the two gas entrance lines was enlarged to 1/2 in (see Fig. 1). The aqueous solutions were prepared in
distilled water by serial dilution of 1 mg mL−1 methanol
solutions of the analytes. The solutions at room temperature (23 ± 1
°C) were pumped through the system by an eight-roll peristaltic pump at
the rate of 2 mL min−1. The capillary membrane was
provided by Dow Corning Co. (Silastic Medical-grade tubing) with a wall
tickness of 0.022 in, an id of 0.025 in, and an od of 0.047 in. The
capillary membrane was expanded by hexane soaking and then fitted to the
1/24 in steel tubes of the DIMP probe; after hexane evaporation, a strong
seal was attained. |
| Fig. 1 Orthogonal cross-sections of the DIMP-T&R-MIMS system: the
highlighted items are: A, DIMP probe; B, capillary membrane loop; C,
filaments; D, ion source block; E, CI gas entrance; F, ceramic probe
adapter; G, focusing lenses; and H, ion source holder. | |
Results and discussion
The DIMP-T&R-MIMS system
Design.. Fig. 1 displays the orthogonal
cross-sections of the DIMP-T&R-MIMS system with the DIMP probe (A) with
a 1/2 in long capillary membrane loop (B) shown in situ in the ion
source (D). In the original T&R-MIMS system10 the membrane and the stainless-steel tubings
were mounted and fixed directly in the source. In the DIMP-T&R-MIMS
system, however, the capillary membrane (B) is fixed into a removable DIMP
probe (A), and a ceramic probe adapter (F) is used to ensure proper
sealing. By finely adjusting the position of the DIMP probe, the membrane
loop (B) can therefore be placed exactly between the two filaments (C) so
as to ensure efficient ionization but particularly faster and more uniform
heating. Heating of the whole membrane loop is actually attained by
rotating the probe, thus slightly de-aligning the membrane loop so as to
allow the upper filament to heat both the external surface of the upper
loop face and the internal surface of the bottom loop face, and the bottom
filament to heat both the external surface of the bottom loop face and the
internal surface of the upper loop face. This uniform heating substantially
reduces memory effects, as discussed below. The removable probe is also
advantageous in other ways: it allows faster membrane replacement since it
eliminates the need for instrument venting; the DIMP probe is only used
when needed, and other standard or MIMS probes can be used and introduced
via the same probe inlet system; the ion source can also be used
for standard MS analysis. Operation.. Similarly to the original T&R-MIMS system,10 the DIMP-T&R-MIMS system can be operated
either in the standard MIMS mode (more suitable for VOC detection)10b or in the T&R-MIMS mode. For SVOC
or combined VOC and SVOC analysis, a room temperature aqueous solution of
the analyte is pumped typically for 10–20 min through the system to
preconcentrate the SVOC inside the membrane, which is kept cold by the
flowing fluid. During the SVOC preconcentration time, VOC analysis is
performed by standard MIMS.1 Then, an air
plug of typically 40 s is introduced (simply by removing the pump tube from
the aqueous sample solution) in the liquid flow. To end the air plug, the
pump tube is introduced into room temperature distilled water, and water is
pumped through the membrane for an additional 40 s. Then, for cleaning, two
40 s air plugs with a 1 min interval are sequentially introduced in the
liquid flow. Signal profile.. Fig. 2 shows a typical signal profile for
DIMP-T&R-MIMS analysis of a 500 ppb aqueous solution of β-naphthol
using selective ion monitoring of the analyte molecular ion of m/z
144. As the solution starts flowing through the system (a), the signal
rises and soon levels off at a relative low intensity, corresponding to the
response for the system in its standard MIMS mode. During the 10 min of
pumping, the SVOC is not efficiently transferred to the gas phase, but it
dissolves, permeates and gets concentrated in the membrane. Then, a 40 s
air plug is introduced (b); when the plug reaches the membrane (c), the
temperature rises rapidly, the preconcentrated SVOCs are thermally and
efficiently released to the gas phase, hence the signal rises and then
drops sharply producing a well-defined, narrow, and for β-naphthol a
nearly 50 times more intense, desorption peak. When the air plug ends (d),
and since room temperature water is now flowing through the system, the
membrane rapidly cools down and the ion signal drops sharply. |
| Fig. 2 DIMP-T&R-MIMS signal profile using selective ion monitoring (SIM)
for 500 ppb aqueous solution of β-naphthol. a, Pumping starts; b, air
plug is introduced in the system; c, air plug reaches the membrane loop; d,
air plug ends; e, first cleaning air plug; and f, second cleaning air
plug. | |
Memory effects.. To clean the membrane of residual SVOCs, two additional 40 s air plugs
with a 1 min separation are introduced just after sample analysis. The
residual SVOCs are removed mostly during the first cleaning air plug (e,
Fig. 2) and cleaning is clearly completed
after the second air plug since the resulting desorption peak (f) is nearly
as abundant as that continuously produced by heating the membrane alone,
that is, from the membrane chemical noise.10aIn the original T&R-MIMS system,10
which used a single filament, the ‘dark’ face of the capillary
membrane was not sufficiently heated during the desorption step. Responses
were therefore not as high and the system was found to be particularly
sensitive to undesirable memory effects.10b The uniform heating of the membrane
loop provided by the DIMP-T&R-MIMS design results in uniform thermal
desorption thus improving sensitivity while reducing memory effects.
Full mass spectra acquisition.. The duration of the DIMP-T&R-MIMS peak is short, but long enough so
as to allow the acquisition of many full mass spectra of the SVOCs; this is
particularly useful for secure analyte identification and mixture analysis.
Fig. 3 shows examples of the full mass
spectra obtained for DIMP-T&R-MIMS analysis at the time of maximal
desorption for aqueous solutions (500 ppb) of three representative SVOCs:
β-naphthol, benzo(a)pyrene, and nicotine. Naturally, however, the more
sensitive selective ion monitoring (SIM) scan mode should be applied for
trace level analysis. |
| Fig. 3 DIMP-T&R-MIMS 70 eV EI mass spectra for 500 ppb aqueous solutions of
(a) β-naphthol; (b) benzo(a)pyrene; and (c) nicotine. Note in (c) the
ion of m/z 149 corresponding to plasticizers present in the
membrane. | |
Other parameters.. Relative and substantial gains (no lower than 50) for several SVOCs,
broad dynamic range, high linearity and reproducibility, and low detection
limits (low to sub ppbs) have been appropriately demonstrated for the
original T&R-MIMS system.10 These
parameters will not be discussed in detail here since our preliminary
results for the new DIMP-T&R-MIMS system have indicated similar
performance. The preliminary results for several SVOCs (β-naphthol,
benzo- (a)pyrene, nicotine, phenanthrene, salicylic acid, lactic acid,
DMSO, and caffeine) as compared to those using a standard MIMS probe14 and to those reported for the original
T&R-MIMS system10 point, however, to a
5–10-fold improved sensitivity (owing likely to the faster and more
uniform heating), and hence, to even lower detection limits of SVOCs in
aqueous solutions when using the new DIMP-T&R-MIMS system. Conclusion
The use of a removable direct insertion membrane probe (DIMP) in a trap
and release membrane introduction mass spectrometry system is shown to be
advantageous. The new DIMP-T&R-MIMS system is more versatile; it can
work efficiently and sequentially in both the standard MIMS and
T&R-MIMS modes for combined VOC and SVOC analysis, and can be used only
when needed, thereby allowing replacement with other MIMS or standard
probes, and the standard operation of the mass spectrometer. With the DIMP
probe, the capillary membrane loop is placed inside the ion source block
exactly between two parallel filaments. Fast and uniform heating of the
membrane loop during the T&R-MIMS thermal desorption step is therefore
accomplished; sensitivity is improved and memory effects are minimized.Acknowledgements
This work has been supported by the Research Support Foundation of the
State of São Paulo (FAPESP) and the Brazilian National Research
Council (CNPq).References
-
(a) T. Kotiaho, F. R. Lauritsen, T. K. Choudhury and R. G. Cooks, Anal. Chem., 1991, 63, 875A CAS;
(b) F. R. Lauritsen and T. Kotiaho, Rev. Anal. Chem., 1996, 237 Search PubMed;
(c) N. Srinivasan, R. C. Johnson, N. Kasthurikrishnan, P. Wong and R. G. Cooks, Anal. Chim. Acta, 1997, 350, 257 CrossRef CAS;
(d) C. S. Creaser, J. W. Stygall and D. J. R. Weston, Anal. Commun., 1998, 35, 9H RSC;
(e) R. C. Johnson,
R. G. Cooks,
T. M. Allen,
M. E. Cisper and
P. H. Hemberger,
Mass Spectrom. Rev., in the
press. Search PubMed.
-
(a) J. A. Shoemaker, T. A. Bellar, J. W. Eichelberger and W. L. Budde, J. Chromatogr. Sci., 1993, 31, 279 CAS;
(b) A. A. Rivlin, Rapid Commun. Mass Spectrom, 1995, 9, 397 CAS;
(c) G. L. Kok, M. E. Cisper and P. H. Hemberger, J. Am. Soc. Mass Spectrom., 1996, 7, 1172 CrossRef CAS.
- M. A. Mendes, R. S. Pimpim, T. Kotiaho and M. N. Eberlin, Anal. Chem., 1996, 68, 3502 CrossRef CAS.
- R. Kostiainen, T. Kotiaho, I. Mattila, M. Ojala and R. A. Ketola, Anal. Chem., 1988, 70, 3028 CrossRef.
-
(a) M. A. Mendes,
R. Sparrapan and
M. N. Eberlin, in
Proceedings of the 46th ASMS Conference on Mass Spectrometry and
Allied Topics, 1998, p. 750;
Search PubMed;
(b) M. A. Mendes,
R. Sparrapan and
M. N. Eberlin,
Anal. Chem., in the press. Search PubMed.
-
(a) S. Bauer and D. Solyom, Anal Chem., 1994, 66, 4422 CrossRef CAS;
(b) M. Soni, S. Bauer, J. W. Amy, P. Wong and R. G. Cooks, Anal Chem., 1995, 67, 1409 CrossRef CAS.
-
(a) M. E. Cisper and P. H. Hemberger, Rapid Commun. Mass Spectrom., 1997, 11, 1449 CrossRef CAS;
(b) N. Kasthurikrishnan, R. G. Cooks and S. Bauer, Rapid Commun. Mass Spectrom., 1996, 10, 751 CrossRef CAS;
(c) R. Alberici, R. Sparrapan, M. N. Eberlin, D. Windmöller and R. Augusti, Anal. Commun., 1999, 36, 221 RSC.
-
(a) M. Ojala, R. A. Ketola, V. Virkki, H. Sorsa and T. Kotiaho, Talanta, 1997, 44, 1253 CrossRef CAS;
(b) T. K. Choudhury, T. Kotiaho and R. G. Cooks, Talanta, 1992, 39, 1113 CrossRef CAS;
(c) R. Alberici,
R. Sparrapan,
M. N. Eberlin and
W. F. Jardim,
Anal. Chem., submitted. Search PubMed.
- L. A. B. Moraes,
M. N. Eberlin,
J. R. Cagnon and
L. H. Urbano,
Anal. Chem., in press. Search PubMed.
-
(a) M. Leth and F. R. Lauritsen, Rapid Commun. Mass Spectrom., 1995, 9, 591 CAS;
(b) F. R. Lauritsen and R. A. Ketola, Anal. Chem., 1997, 69, 4917 CrossRef CAS.
- G. Matz and F. Lennemann, J. Chromatogr. A, 1996, 750, 141 CrossRef CAS.
-
Laser desorption of SVOCs from the membrane has also been successful, see:
(a) M. H. Soni, A. P. Baronavski and S. W. McElvany, Rapid Commun. Mass Spectrom., 1998, 12, 1635 CrossRef CAS;
(b) M. H. Soni, J. H. Callahan and S. W. McElvany, Anal. Chem., 1998, 70, 3103 CrossRef CAS.
-
(a) M. E. Bier and R. G. Cooks, Anal. Chem., 1987, 59, 597 CrossRef CAS;
(b) M. E. Bier, T. Kotiaho and R. G. Cooks, Anal. Chim. Acta, 1990, 231, 175 CrossRef CAS.
-
(a) M. A. Mendes, R. S. Pimpim, T. Kotiaho, J. S. Barone and M. N. Eberlin, Quim. Nova, 1996, 19, 480 Search PubMed;
(b) R. F. P. Nogueira, R. M. Alberici, M. A. Mendes, W. F. Jardim and M. N. Eberlin, Ind. Eng. Chem. Res.,, 1999, 38, 1754 CrossRef CAS.
|
This journal is © The Royal Society of Chemistry 2000 |
Click here to see how this site uses Cookies. View our privacy policy here.