Anal. Chem. 2000, 72, 3553-3562
Interpretation of Mass Spectra from Organic Compounds in Aerosol Time-of-Flight Mass Spectrometry Philip J. Silva and Kimberly A. Prather*
Department of Chemistry, University of California, Riverside, California 92521
Organic compounds containing a variety of functional groups have been analyzed using aerosol time-of-flight mass spectrometry. Both positive and negative laser desorption/ionization mass spectra have been acquired for compounds of relevance to ambient air particulate matter, including polycyclic aromatic hydrocarbons, heterocyclic analogues, aromatic oxygenated compounds such as phenols and acids, aliphatic dicarboxylic acids, and reduced nitrogen species such as amines. In many cases, positive ion mass spectra are similar to those found in libraries for 70-eV electron impact mass spectrometry. However, formation of even-electron molecular ions due to adduct formation also plays a major role in ion formation. Negative ion mass spectra suggest that organic compounds largely disintegrate into carbon cluster fragments (Cn- and CnH-). However, information about the heteroatoms present in organic molecules, especially nitrogen and oxygen, is carried dominantly by negative ion spectra, emphasizing the importance of simultaneous analysis of positive and negative ions in atmospheric samples. The introduction of a number of real-time single-particle mass spectrometry (RTSPMS) techniques1-6 offers the potential for analysis of aerosol composition and characterization of processes that have eluded analysis for a variety of reasons. These techniques have shown their utility for analysis of source emissions7 and ambient analysis of particles in the troposphere.8-12 In (1) Noble, C. A.; Prather, K. A. Environ. Sci. Technol. 1996, 30, 2667-2680. (2) Hinz, K.-P.; Kaufmann, R.; Spengler, B. Aerosol Sci. Technol. 1996, 24, 233242. (3) Carson, P. G.; Johnston, M. V.; Wexler, A. S. Rapid Commun. Mass Spectrom. 1997, 11, 993-996. (4) Yang, M.; Reilly, P. T. A.; Boraas, K. B.; Whitten, W. B.; Ramsey, J. M. Rapid Commun. Mass Spectrom. 1996, 10, 347-351. (5) Murphy, D. M.; Thomson, D. S. Aerosol Sci. Technol. 1995, 22, 237-249. (6) Kievit, O.; Weiss, M.; Verheijen, P. J. T.; Marijnissen, J. C. M.; Scarlett, B. Chem. Eng. Commun. 1996, 151, 79-100. (7) Silva, P. J.; Prather, K. A. Environ. Sci. Technol. 1997, 31, 3074-3080. (8) Gard, E. E.; Kleeman, M. J.; Gross, D. S.; Hughes, L. S.; Allen, J. O.; Morrical, B. D.; Fergenson, D. P.; Dienes, T.; Gaelli, M.; Cass, G. R.; Prather, K. A. Science 1998, 279, 1184-1187. (9) Liu, D.-Y.; Rutherford, D.; Kinsey, M.; Prather, K. A. Anal. Chem. 1997, 69, 1808-1814. (10) Murphy, D. M.; Thomson, D. S. J. Geophys. Res. 1997, 102, 6353-6368. (11) Murphy, D. M.; Thomson, D. S. J. Geophys. Res. 1997, 102, 6341-6352. (12) Murphy, D. M.; Thomson, D. S.; Mahoney, M. J. Science 1998, 282, 16641669. 10.1021/ac9910132 CCC: $19.00 Published on Web 06/24/2000
© 2000 American Chemical Society
addition, other unique applications have been explored.13-15 However, the use of these techniques for the analysis of organic compounds in aerosols has been limited because of a lack of knowledge regarding the desorption/ionization and fragmentation processes in the techniques and by the complex mixture of organic species present in atmospheric particles. There is great potential for applying RTSPMS techniques for the analysis of the organic components of atmospheric aerosols. There is a need for on-line analysis techniques for organics because of the limitations of traditional analytical techniques. Data on the presence of semivolatile organic compounds in aerosols can be lost due to volatilization of the compounds after collection on filter media prior to chemical analysis. In addition, many highly polar compounds cannot be readily analyzed using the available suite of off-line techniques such as gas chromatography. Previous work using laser microprobe mass analysis (LAMMA), the off-line forerunner to these real-time techniques, has elucidated some aspects of the ionization and fragmentation mechanisms observed using laser desorption/ionization.16-20 However, to date there has been no investigation of the capability of RTSPMS techniques for analysis of the wide range of compounds known and expected to be present in atmospheric particles. The purpose of this study is to understand and identify potential characteristic ion peaks in the mass spectra of various relevant compounds and compound classes expected to be present in atmospheric particulate matter. EXPERIMENTAL SECTION An aerosol time-of-flight mass spectrometer (ATOFMS) provides size and chemical composition information for individual particles. It operates in a continuous sampling manner, allowing for real-time analysis of particles with high time resolution. The (13) Noble, C. A.; Prather, K. A. Aerosol Sci. Technol. 1998, 29, 294-306. (14) Middlebrook, A. M.; Thomson, D. S.; Murphy, D. M. Aerosol Sci. Technol. 1997, 27, 293-307. (15) Ge, Z.; Wexler, A. S.; Johnston, M. V. J. Colloid Interface Sci. 1996, 183, 68-77. (16) Van Vaeck, L.; Claereboudt, J.; De Waele, J.; Esmans, E.; Gijbels, R. Anal. Chem. 1985, 57, 2944-2951. (17) Hercules, D. M.; Novak, F. P.; Viswanadham, S. K.; Wilk, Z. A. Anal. Chim. Acta 1987, 195, 61-71. (18) Van Vaeck, L.; Bennett, J.; Van Epsen, P.; Schweikert, E.; Gijbels, R.; Adams, F.; Lauwers, W. Org. Mass Spectrom. 1989, 24, 782-796. (19) Van Vaeck, L.; Bennett, J.; Van Epsen, P.; Schweikert, E.; Gijbels, R.; Adams, F.; Lauwers, W. Org. Mass Spectrom. 1989, 24, 797-806. (20) Van Vaeck, L.; De Waele, J.; Gijbels, R. Mikrochim. Acta 1984, III, 237257.
Analytical Chemistry, Vol. 72, No. 15, August 1, 2000 3553
instrumental setup has been described in detail previously.21-23 Particles are introduced into the instrument through a nozzle and undergo a supersonic expansion. The particles are accelerated to a terminal velocity that is proportional to their aerodynamic diameter. The particles then enter a sizing region where they pass through two continuous wave laser beams. Scattering signals are collected as each particle passes through each laser beam. This measures a particle time of flight that can be converted to aerodynamic size with a calibration curve. After being sized, the particle travels to the ion source region of a time-of-flight mass spectrometer. Chemical species in the particle are desorbed/ ionized, using the pulsed output from an ultraviolet laser, and separated and detected using a reflectron time-of-flight mass spectrometer equipped with multichannel plates (MCPs) for ion detection. The experiments described in this paper were performed using the laboratory-based ATOFMS.1,24 An argon ion laser (488- and 514-nm continuous wave output) was used for the aerodynamic sizing region of the instrument, with size calibrations indicating a lower size limit of 0.3 µm for these experiments. Laser desorption/ionization of chemical species in the particles was accomplished using a Nd:YAG laser operating at 266 nm. Positive and negative ions were acquired separately by changing the applied voltages for the source and reflectron regions of the timeof-flight mass spectrometer. Several different particle generation techniques were used. Solid samples were ground into a fine powder and the resulting particles were suspended in a small glass bottle. This sampling apparatus was connected to the inlet of the instrument, resulting in the detection and analysis of large particles up to ∼8.0 µm, depending on the fineness of the suspended powder. Liquid samples were analyzed using a home-built atomizer for generation of particles. A limited number of experiments made use of acidbase reactions in order to form particles of organic salts. In these experiments, gas-phase acids and bases were introduced into the glass bottle and the resulting particles were analyzed by ATOFMS. Mixtures of organic compounds were analyzed both by the suspension of homogeneous powders and using a vibrating orifice aerosol generator (VOAG, TSI model 3450) for creation of particles containing mixtures of more than one chemical species. In all cases, mixtures of 1:1 mole ratios were prepared. Laser energy for the desorption/ionization laser was varied for each compound between approximately 5 and 40 mJ with a spot size of ∼0.75 mm, representing typical values used during acquisition of ambient data. This translates into a laser fluence of approximately 108-109 W cm-2. However, due to inhomogeneities in the laser beam, the actual fluence for desorption/ionization from one shot to another can vary considerably. A minimum of 100 positive and negative ion spectra were acquired for each compound or mixture. Spectra chosen for display represent averages of those acquired using both high (109 W cm-2) and low (108 W cm-2) laser fluence. The terms “low” and “high” are used as relative terms for this experiment; however, it is important to note that ions can be formed at even lower fluences, down to a (21) Gard, E.; Mayer, J. E.; Morrical, B. D.; Dienes, T.; Fergenson, D. P.; Prather, K. A. Anal. Chem. 1997, 69, 4083-4091. (22) Nordmeyer, T.; Prather, K. A. Anal. Chem. 1994, 66, 3540-3542. (23) Prather, K. A.; Nordmeyer, T.; Salt, K. Anal. Chem. 1994, 66, 1403-1407. (24) Salt, K.; Noble, C. A.; Prather, K. A. Anal. Chem. 1996, 68, 230-234.
3554 Analytical Chemistry, Vol. 72, No. 15, August 1, 2000
Table 1. Polycyclic Aromatic Hydrocarbons and Oxygenated/Aza Polycyclics Analyzed Using ATOFMS compound
MW
CAS registry no.
naphthalene acenaphthene 1,5-dihydroxynaphthalene fluorene phenanthrene phenanthridine 9-fluorenone perinaphthenone fluoranthene pyrene 2-methylanthraquinone phenanthraquinone chrysene perylene benzo[ghi]perylene coronene
128 154 160 166 178 179 180 180 202 202 208 222 228 252 276 300
91-20-3 83-32-9 83-56-7 86-73-7 85-01-8 229-87-8 486-25-9 548-39-0 206-44-0 129-00-0 84-54-8 84-11-7 218-01-9 198-55-0 191-24-2 191-07-1
threshold value of 106 W cm-2. The experiments presented in this paper were conducted at the chosen fluences to reproduce and gain insight into mass spectra acquired at typical powers used in previous field studies conducted with ATOFMS. This shows both the parent ion region (important at low laser fluence) and fragments from the compounds (important at high laser fluence). In a number of cases, spectra of pure organic compounds also show peaks due to alkali metals such as sodium and potassium, due to the extremely high sensitivity of ATOFMS to these elements that are present as trace impurities (
