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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.

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