3. FOOD ChEMISTRy & bIOTEChNOLOGy 3.1. Lectures
3. FOOD ChEMISTRy & bIOTEChNOLOGy 3.1. Lectures
3. FOOD ChEMISTRy & bIOTEChNOLOGy 3.1. Lectures
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Chem. Listy, 102, s265–s1311 (2008) Food Chemistry & Biotechnology<br />
L10 APPLICATION POTENTIAL OF NOVEL GAS<br />
ChROMATOGRAPhy hIGh ThROuGhPuT<br />
TIME-OF-FLIGhT MASS SPECTROMETERy<br />
SySTEM (TRu TOF) IN <strong>FOOD</strong> AND<br />
ENVIRONMENTAL ANALySIS<br />
JAKUB SCHůREK, JAnA PULKRABOVá and JAnA<br />
HAJŠLOVá<br />
Department of Food Chemistry and Analysis, Faculty of Food<br />
and Biochemical Technology, Institute of Chemical Technology,<br />
Technická 5, Praha 166 28, Czech Republic,<br />
jakub.schurek@vscht.cz<br />
Introduction<br />
In last years, analytical approaches employing gas chromatography<br />
coupled to time-of-flight mass spectrometry<br />
(GC-TOF MS) proved to be a useful tool in assessment of<br />
quality and safety of food 1–4 and also environmental matrices<br />
5 . But only recently, at the end of 2007, new time-of-flight<br />
mass spectrometric (TOF MS) detector specialy designed for<br />
high-throughput of samples, has been introduced. High throughput<br />
is the key to increased profitability of the analyses,<br />
while obtaining faster results and optimization. The need for<br />
selected ion monitoring (SIM) operation and low dynamic<br />
range associated with traditional quadrupoles and ion traps<br />
may take time and money away from laboratory’s bottomline.<br />
The assessed instrument (GC-HT TOF MS) is combining<br />
fast acquisition mass spectrometer (80 Hz) with specific<br />
data-mining algorithms. The aim of this benchtop instrumental<br />
set-up is to achieve the speed and resolution necessary<br />
to accomplish Time-Compressed Chromatography. Using<br />
such detector, sufficient data density is obtained to accurately<br />
characterize even the narrowest GC peaks produced under<br />
conditions of fast chromatography separation. The acquisition<br />
of the full mass spectral information of the sample with<br />
comparable sensitivity as obtained by selected ion monitoring<br />
(SIM) mode with quadrupole or ion trap instruments makes<br />
feasible the application of a deconvolution algorithm obtaining<br />
pure mass spectra even for coeluting compounds and<br />
achieving reliable confirmation. Consequently, trace level<br />
analysis of unknown sample components can be performed.<br />
The schematic view of GC-HT TOF MS is shown in<br />
Figure 1. Within the mass spectrometer source, the filament<br />
continuously generates an electron beam. The GC effluent<br />
is introduced into the source through a heated transfer line.<br />
Electron ionization (EI) occurs as a result of interactions<br />
between an electron beam with an analyte molecule from the<br />
GC effluent. Chemical ionization (CI) occurs as a result of EI<br />
interactions between the electron beam with the CI reagent<br />
gas which creates charged reagent ions that ionize the analyte<br />
molecules from the GC effluent. Ions are pulsed from the orthogonal<br />
accelerator at a nominal frequency of 20 kHz. Each<br />
pulse of ions into the flight tube results in a mass spectrum<br />
which is referred to as a transient. The transients are then<br />
summed to provide mass spectral acquisition rates up to<br />
80 spectra second –1 . The focusing optics are used to direct<br />
s564<br />
ions through the system and ensure a high recovery of signal<br />
at the detector. Deflection optics are used to prevent unwanted<br />
signals, such as ions from a solvent front or unwanted background<br />
ions generated by carrier gas or residual gas, and<br />
extend the life of the detector. The ions are pulsed into the<br />
flight tube with equal kinetic energies (K.E. = 1/2 mv 2 ).<br />
Therefore, ions of varying mass-to-charge ratios will have<br />
different velocities as they move through the flight tube.<br />
Fragment ions with different velocities traveling over the<br />
same fixed distance will have different arrival times at the<br />
end of that distance (velocity = distance/time). Masses are<br />
resolved in time-of-flight mass spectrometers by the time<br />
each mass takes to reach the detector at the end of the flight<br />
path (time = constant x m 1/2 ). For example, a mass of 100 mu<br />
will take approximately 15 microseconds to reach the detector<br />
while a mass of 1,000 mu will take 50 microseconds to<br />
travel the same distance.<br />
In this work we aimed to evaluate new GC-HT TOF<br />
MS instrumentation in analysis of pesticides, pharmaceuticals,<br />
poly-chlorinated biphenyls (PCBs) and poly-brominated<br />
dibenzo ethers (PBDEs). The best GC-MS settings has<br />
been optimized in order to obtaine fast and reliable analytical<br />
methods for routine control of purified extracts of different<br />
food-stuffs, or sediment, and water. Appraisal of mentioned<br />
technique with respect to the cost and time demands was also<br />
done.<br />
Fig. 1. Schematic diagram of GC-hT TOF MS<br />
Experimental<br />
R e a g e n t s a n d M a t e r i a l<br />
Tested compounds (listed in Table II) with purity ranging<br />
from 95 to 99 % were purchased from Dr. Ehrenstorfer<br />
(Augsburg, Germany) in case of pesticides and PCBs.<br />
PBDEs and estrogenic pharmaceuticals were obtained from<br />
Cambridge Isotope Laboratories (CIL, UK). All solvents<br />
used within sample preparation (see Table I) were of analytical<br />
grade (Scharlau, Barcelona, Spain). Working solutions<br />
(concentration 1.25–250 µg dm –3 ) were prepared by series of<br />
dilutions of the stock solutions (10 mg dm –3 ) with appropriate<br />
solvent.