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Proton-transfer-reaction mass spectrometry (PTR-MS) is a very sensitive technique for online monitoring of volatile organic compounds (VOCs) in ambient air developed by scientists at the Institut für Ionenphysik at the Leopold-Franzens University in Innsbruck, Austria. A PTR-MS instrument consists of an ion source that is directly connected to a drift tube (in contrast to SIFT-MS no mass filter is interconnected) and an analyzing system (quadrupole mass analyzer or time-of-flight mass spectrometer). Commercially available PTR-MS instruments have a response time of about 100 ms and reach a detection limit in the single digit pptv region. Established fields of application are environmental research, food and flavour science, biological research, medicine, etc.

Theory
With H3O+ as the primary ion the proton transfer process is (with $$R$$ being the trace component)
 * $$H_3O^+ + R \longrightarrow RH^+ + H_2O$$ (1).

Reaction (1) is only possible if energetically allowed, i.e. if the proton affinity of $$R$$ is higher than the proton affinity of H2O (691 kJ/mol ). As most components of ambient air possess a lower proton affinity than H2O (e.g. N2, O2, Ar, CO2, etc.) the H3O+ ions only reacts with VOC trace components and the air itself acts as a buffer gas. Moreover due to the low number of trace components one can assume that the total number of H3O+ ions remains nearly unchanged, which leads to the equation
 * $$\lbrack RH^+\rbrack = \lbrack H_3O^+\rbrack_0 \left (1-e^{-k\lbrack R\rbrack t}\right )\approx \lbrack H_3O^+\rbrack _0 \lbrack R\rbrack kt$$ (2).

In equation (2) $$\lbrack RH^+\rbrack$$ is the density of product ions, $$\lbrack H_3O^+\rbrack_0$$ is the density of primary ions in absence of reactant molecules in the buffer gas, $$k$$ is the reaction rate constant and $$t$$ is the average time the ions need to pass the reaction region. With a PTR-MS instrument the number of product and of primary ions can be measured, the reaction rate constant can be found in literature for most substances and the reaction time can be derived from the set instrument parameters. Therefore the absolute concentration of trace constituents $$\lbrack R\rbrack$$ can be easily calculated without the need of calibration or gas standards. Furthermore it gets obvious that the overall sensitivity of a PTR-MS instrument is mainly dependent on the primary / reagent ion yield. Fig. 1 gives an overview of several published (in peer-reviewed journals) reagent ion yields during the last decades and the corresponding sensitivities.

Technology
In commercial PTR-MS instruments water vapour is ionized in a hollow cathode discharge:
 * $$e^- + H_2O \longrightarrow H_2O^+ + 2e^-$$
 * $$e^- + H_2O \longrightarrow H_2^+ + O + 2e^-$$
 * $$e^- + H_2O \longrightarrow H^+ + OH + 2e^-$$
 * $$e^- + H_2O \longrightarrow O^+ + H_2 + 2e^-$$.

After the discharge a short drift tube is used to form very pure (>99.5% ) H3O+ via ion-molecule reactions:
 * $$H_2^+ + H_2O \rightarrow H_2O^+ + H_2$$
 * $$H^+ + H_2O \rightarrow H_2O^+ + H$$
 * $$O^+ + H_2O \rightarrow H_2O^+ + O$$
 * $$H_2O^+ + H_2O \longrightarrow H_3O^+ + OH$$.

Due to the high purity of the primary ions a mass filter between the ion source and the reaction drift tube is not necessary and the H3O+ ions can be injected directly. The absence of this mass filter in turn greatly reduces losses of primary ions and leads eventually to an outstandingly low detection limit of the whole instrument. In the reaction drift tube a vacuum pump is continuously drawing through air containing the VOCs one wants to analyze. At the end of the drift tube the protonated molecules are mass analyzed (Quadrupole mass analyzer or Time-of-flight mass spectrometer) and detected.

Advantages of PTR-MS

 * Low fragmentation: Only a small amount of energy is transferred during the ionization process (compared to e.g. electron impact ionization), therefore fragmentation is suppressed and the obtained mass spectra are easily interpretable.
 * No sample preparation is necessary: VOC containing air and fluids headspaces can be analyzed directly.
 * Real-time measurements: With a typical response time of 100 ms VOCs can be monitored on-line.
 * Real-time quantification: Absolute concentrations are obtained directly without previous calibration measurements.
 * Compact and robust setup: Due to the simple design and the low number of parts needed for a PTR-MS instrument, it can be built in into space saving and even mobile housings.
 * Easy to operate: For the operation of a PTR-MS only electric power and a small amount of distilled water are needed. Unlike other techniques no gas cylinders are needed for buffer gas or calibration standards.

Disadvantages of PTR-MS and countermeasures

 * Not all molecules detectable: Because only molecules with a proton affinity higher than water can be detected by PTR-MS, proton transfer from H3O+ is not suitable for all fields of application. Therefore in 2009 first PTR-MS instruments were presented, which are capable of switching between H3O+ and O2+ (and NO+) as reagent ions . This enhances the number of detectable substances to important compounds like ethylene, acetylene, most halocarbons, etc. In 2012 a PTR-MS instrument was introduced which extends the selectable reagent ions to Kr+ and Xe+ ; this should allow for the detection of nearly all possible substances (up to the ionization energy of krypton (14 eV )). Although the ionization method for these additional reagent ions is charge-exchange rather than proton-transfer ionization the instruments can still be considered as "classic" PTR-MS instruments, i.e. no mass filter between the ion source and the drift tube and only some minor modifications on the ion source and vacuum design.
 * Maximum measurable concentration limited: Equation (2) is based on the assumption that the decrease of primary ions is negligible, therefore the total concentration of VOCs in air must not exceed about 10 ppmv. Otherwise the instrument's response will not be linear anymore and the concentration calculation will be incorrect. This limitation can be overcome easily by diluting the sample with a well-defined amount of pure air.

Applications
The most common applications for the PTR-MS technique are (including some relevant publications):
 * Environmental research
 * Waste incineration
 * Food and flavour science
 * Biological research
 * Process monitoring
 * Indoor air quality
 * Medicine and biotechnology
 * Homeland Security

Extensive reviews about PTR-MS and some of its applications were published in Mass Spectrometry Reviews by Joost de Gouw et al. (2007) and in Chemical Reviews by R.S. Blake et al. (2009). A special issue of the Journal of Breath Research dedicated to PTR-MS applications in medical research was published in 2009.

Food Science
Fig. 2 shows a typical PTR-MS measurement performed in food and flavor research. The test person swallows a sip of a vanillin flavored drink and breathes via his nose into a heated inlet device coupled to a PTR-MS instrument. Due to the high time resolution and sensitivity of the instrument used here, the development of vanillin in the person's breath can be monitored in real-time (please note that isoprene is shown in this figure because it is a product of human metabolism and therefore acts as an indicator for the breath cycles). The data can be used for food design, i.e. for adjusting the intensity and duration of vanillin flavor tasted by the consumer.

Another example for the application of PTR-MS in food science was published in 2008 by C. Lindinger et al. in Analytical Chemistry. This publication found great response even in non-scientific media. Lindinger et al. developed a method to convert "dry" data from a PTR-MS instrument that measured headspace air from different coffee samples into expressions of flavour (e.g. "woody", "winey", "flowery", etc.) and showed that the obtained flavor profiles matched nicely to the ones created by a panel of European coffee tasting experts.

Air quality analysis
In Fig. 3 a mass spectrum of air inside a laboratory (obtained with a time-of-flight (TOF) based PTR-MS instrument), is shown. The peaks on masses 19, 37 and 55 m/z (and their isotopes) represent the reagent ions (H3O+) and their clusters. On 30 and 32 m/z NO+ and O2+, which are both impurities originating from the ion source, appear. All other peaks correspond to compounds present in typical laboratory air (e.g. high intensity of protonated acetone on 59 m/z). If one takes into account that virtually all peaks visible in Fig. 3 are in fact double, triple or multiple peaks (isobaric compounds) it becomes obivious that for PTR-MS instruments selectivity is at least as important as sensitivity, especially when complex samples / compositions are analyzed. Methods to handle this issue have been suggestested in literature as:


 * High mass resolution: When the PTR source is coupled to a high resolution mass spectrometer isobaric compounds can be distinguished and substances can be identified via their exact mass.


 * Switchable reagent ions: Some PTR-MS instruments are despite of the lack of a mass filter between the ion source and the drift tube capable of switching the reagent ions (e.g. to NO+ or O2+). With the additional information obtained by using different reagent ions a much higher level of selectivity can be reached, e.g. some isomeric molecules can be distinguished.

Manufacturer

 * Ionicon Analytik GmbH
 * Kore Technology Ltd

Category:Mass spectrometry Category:Measuring instruments