Thermal decomposition products of butyraldehyde Courtney D. Hatten, Kevin R. Kaskey, Brian J. Warner, Emily M. Wright, and Laura R. McCunn Citation: The Journal of Chemical Physics 139, 214303 (2013); doi: 10.1063/1.4832898 View online: http://dx.doi.org/10.1063/1.4832898 View Table of Contents: http://scitation.aip.org/content/aip/journal/jcp/139/21?ver=pdfcov Published by the AIP Publishing This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 THE JOURNAL OF CHEMICAL PHYSICS 139, 214303 (2013) Thermal decomposition products of butyraldehyde Courtney D. Hatten, Kevin R. Kaskey, Brian J. Warner, Emily M. Wright, and Laura R. McCunna) Department of Chemistry, Marshall University, Huntington, West Virginia 25755, USA (Received 12 August 2013; accepted 8 November 2013; published online 2 December 2013) The thermal decomposition of gas-phase butyraldehyde, CH3 CH2 CH2 CHO, was studied in the 1300– 1600 K range with a hyperthermal nozzle. Products were identified via matrix-isolation Fourier transform infrared spectroscopy and photoionization mass spectrometry in separate experiments. There are at least six major initial reactions contributing to the decomposition of butyraldehyde: a radical decomposition channel leading to propyl radical + CO + H; molecular elimination to form H2 + ethylketene; a keto-enol tautomerism followed by elimination of H2 O producing 1-butyne; an intramolecular hydrogen shift and elimination producing vinyl alcohol and ethylene, a β–C–C bond scission yielding ethyl and vinoxy radicals; and a γ –C–C bond scission yielding methyl and CH2 CH2 CHO radicals. The first three reactions are analogous to those observed in the thermal decomposition of acetaldehyde, but the latter three reactions are made possible by the longer alkyl chain structure of butyraldehyde. The products identified following thermal decomposition of butyraldehyde are CO, HCO, CH3 CH2 CH2 , CH3 CH2 CH=C=O, H2 O, CH3 CH2 C≡CH, CH2 CH2 , CH2 =CHOH, CH2 CHO, CH3 , HC≡CH, CH2 CCH, CH3 C≡CH, CH3 CH=CH2 , H2 C=C=O, CH3 CH2 CH3 , CH2 =CHCHO, C4 H2 , C4 H4 , and C4 H8 . The first ten products listed are direct products of the six reactions listed above. The remaining products can be attributed to further decomposition reactions or bimolecular reactions in the nozzle. © 2013 AIP Publishing LLC. [http://dx.doi.org/10.1063/1.4832898] I. INTRODUCTION Aldehydes are commonly formed when hydrocarbons are present in environments of high temperatures and low oxygen content. Examples include the production and combustion of biofuels as well as cigarette smoking and coffee roasting.1–5 Low molecular weight aldehydes such as butyraldehyde (CH3 CH2 CH2 CHO) are known byproducts of the pyrolysis of biomass which occurs in the initial steps in the production of some biofuels.1 Trace amounts of butyraldehyde have been identified in bio-oil using gas chromatography-mass spectrometry.2 Butyraldehyde has also been detected via gas chromatography and mass spectrometry following the pyrolysis of cigarette ingredients such as n-butyl alcohol and white sugar.3, 4 The pyrolytic environment of a lit cigarette can cause further breakdown of the aldehyde byproducts found in tobacco. Coffee brewing has been proven to emit aldehydes as odorous fumes.5 The trace amounts of butyraldehyde emitted during this process can thermally decompose during the completion of brewing. During the pyrolysis of biomass, cigarette ingredients, and coffee, as well as the combustion of bio-oil, aldehyde byproducts are exposed to high temperatures and can undergo thermal decomposition reactions. Understanding the thermal decomposition pathways of butyraldehyde would facilitate the prediction of pollutants or contaminants in the processes described above. Decomposition of various aldehydes has been studied previously with the use of shock tubes and flow reactors.6–8 To a) Author to whom correspondence should be addressed. Electronic mail: [email protected] 0021-9606/2013/139(21)/214303/9/$30.00 our knowledge, no thermal decomposition studies have been performed on butyraldehyde, but insight can be gained by examining the known thermal decomposition pathways of simpler aldehydes such as acetaldehyde. Vasiliou and co-workers identified the products of acetaldehyde pyrolysis using matrix-isolation Fourier transform infrared spectroscopy.9, 10 They also presented complimentary experiments using photoionization mass spectrometry (PIMS) to detect the pyrolysis products. The unimolecular pathways for acetaldehyde that were originally proposed are CH3 CHO + → CH3 + [HCO] → CH3 + H + CO(radical decomposition), CH3 CHO + → H2 + CH2 =C=O (elimination), (1) (2) CH3 CHO + → [CH2 =CH − OH] → HC≡CH + H2 O(isomerization/elimination). (3) While products from all three pathways were observed, Vasiliou and co-workers discovered that some of the products came from bimolecular reactions.10 They repeated the pyrolysis experiments on a 50:50 mixture of isotopically labeled acetaldehyde (CD3 CDO) and unlabeled acetaldehyde (CH3 CHO) and detected the products using PIMS. This experiment resulted in isotopically scrambled products, containing both deuterium and hydrogen. If the products were formed from a unimolecular pathway, then they would have either deuterium or hydrogen, not both. After ruling out wall reactions within the hyperthermal nozzle, it was concluded that bimolecular 139, 214303-1 © 2013 AIP Publishing LLC This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-2 Hatten et al. J. Chem. Phys. 139, 214303 (2013) reactions must occur during pyrolysis under their experimental conditions. Pyrolysis reactions of butyraldehyde can be hypothesized based on the reactions observed in acetaldehyde by Vasiliou and co-workers.9 The thermal decomposition mechanisms of acetaldehyde and butyraldehyde at high temperatures should be similar, but it is conceivable that butyraldehyde may have additional reaction pathways due to its longer alkyl chain. For example, there is a known mechanism11–13 for butyraldehyde forming a cyclic intermediate where the oxygen abstracts a γ -hydrogen from the terminal carbon, followed by the elimination of ethylene. Small aldehydes such as propionaldehyde and acetaldehyde cannot access such a reaction pathway because their alkyl chains are too short to form the cyclic intermediate and bring the oxygen atom in close proximity to a terminal hydrogen. Also, the C–C bonds in the β and γ positions relative to the carbonyl group have bond energies similar to the α C–C bond.14 While a literature search has not indicated any previous observation of reactions involving such bond ruptures, they should be considered in the potential mechanism. In summary, the main reactions expected in the thermal decomposition of butyraldehyde are CH3 CH2 CH2 CHO + → CH3 CH2 CH2 + CO + H (radical decomposition), (4) CH3 CH2 CH2 CHO + → CH3 CH2 CH=C=O + H2 (elimination), (5) CH3 CH2 CH2 CHO + → CH3 CH2 C≡CH + H2 O (isomerization/elimination), (6) CH3 CH2 CH2 CHO + → CH2 =CH2 + CH2 =C(H)OH (H−shift/elimination), (7) CH3 CH2 CH2 CHO + → CH3 CH2 + CH2 CHO (β−C − C scission), (8) CH3 CH2 CH2 CHO + → CH3 + CH2 CH2 CHO (γ −C − C scission). (9) Comparing the decomposition of butyraldehyde to that of acetaldehyde may show the influence of the size of the alkyl chain on the reaction pathways. The purpose of the experiments presented here is to identify the products of butyraldehyde pyrolysis by using a hyperthermal nozzle (Chen nozzle)15–17 and matrix-isolation Fourier transform infrared (FTIR) spectroscopy. The hyperthermal nozzle provided an oxygen-free environment for thermal decomposition of gas-phase butyraldehyde, while matrixisolation FTIR was used to detect the products. Additionally, PIMS of the pyrolysis products were measured in order to complement the FTIR spectra and identify products that are difficult to detect by FTIR. An advantage of the experiments presented here is that they probe reactions occurring relatively early in the pyrolysis process. The typical residence time for a butyraldehyde molecule in the high-temperature region of the pyrolyzer is on the order of 50–100 μs.9, 15 The expansion of pyrolysis products leaving the high-temperature tube rapidly cools the products and quenches any reactions. Therefore, it is possible to detect and identify radical intermediates or products that occur in the pyrolysis mechanism. II. EXPERIMENTAL METHODS Thermal decomposition of butyraldehyde (purity ≥99.5%; Sigma Aldrich) was accomplished via a hyperthermal nozzle that has been described elsewhere in the literature.15 A matrix mixture (0.2%–0.33%) of butyraldehyde in argon totaling approximately 700 Torr was prepared using standard manometric techniques. The mixture was expanded from a pulsed valve (General Valve Series 9) operating at 40 Hz into the 1.5 in. × 1 mm silicon carbide (SiC) tube which was resistively heated. The temperature of the SiC tube was controlled using a Series 16A temperature controller made by Love controls. The pyrolysis products were sprayed out of the tube and onto a cesium iodide (CsI) window mounted in a cryostat (Janis Research) with a base pressure of 1.0 × 10−6 Torr. The CsI window was cooled to 15 K by a closed-cycle helium refrigerator (Sumitomo Heavy Industries Ltd.) and regulated by a Lake Shore 331 Temperature Controller. The pyrolysis products were isolated in an Ar matrix and then cooled to 4 K prior to FTIR analysis. FTIR spectra were collected for 120 scans with 0.5 cm−1 resolution with a Bruker Vertex 70 spectrometer that was purged with nitrogen gas. Photoionization mass spectrometry was also performed following the pyrolysis of butyraldehyde in separate experiments. A pyrolysis nozzle identical to the one described above was mounted on a photoionization mass spectrometer which has been described previously.15 A mixture of 0.3% butyraldehyde in 2 atm of helium was expanded through the pyrolysis nozzle (1300–1600 K) into a 10−5 Torr vacuum chamber and passed through a skimmer (3 mm diameter). The resultant beam was crossed with a vacuum ultraviolet (VUV) (118.2 nm) laser operating at 30 Hz, ∼0.5 μJ/pulse. The VUV light was generated by tripling the 3rd harmonic of an Nd:YAG in an argon cell. Products from thermal decomposition of butyraldehyde were ionized and then mass analyzed by a reflectron time of flight (TOF) mass spectrometer. Ions were detected by a channeltron and the signal was collected by a Tektronix digital oscilloscope. III. RESULTS AND DISCUSSION A list of all the products observed following pyrolysis of butyraldehyde appears in Table I. PIMS analysis was performed following pyrolysis of butyraldehyde at various SiC tube temperatures in order to confirm the presence of the species found in the FTIR spectra, as well as to detect species that were not discernible by matrix-isolation FTIR. The PIMS spectra at 300 K, 1300 K, 1500 K, and 1600 K are shown in Figure 1. The use of two separate detection techniques proved This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-3 Hatten et al. J. Chem. Phys. 139, 214303 (2013) TABLE I. Summary of all products observed following the pyrolysis of butyraldehyde at 1300–1600 K, listed in order of molecular weight. Checkmarks indicate evidence observed for each product. A question mark indicates an assignment that is ambiguous or lacks sufficient signal to be certain. Product CH3 H2 O HCCH CH2 CH2 CO HCO CH2 CCH CH3 CCH CH3 CHCH2 H2 CCO H2 CCHO CH3 CH2 CH2 CH2 CHOH CH3 CH2 CH3 C4 H2 C4 H4 CH3 CH2 C≡CH CH2 CHCHO C4 H8 CH3 CH2 CHCO CH3 CH2 CHCHOH PIMS Matrixisolation FTIR Comments ? ? ? ? ? IE prohibits PIMS detection IE prohibits PIMS detection IE prohibits PIMS detection ? ? ? ? IE prohibits PIMS detection No literature comparison for MI-FTIR advantageous in several cases, for example, detection of the methyl radical (ionization energy, IE = 9.8).18 CH3 + appears at m/z = 15 in Figure 1. The methyl radical is expected to exhibit the highest FTIR absorption at 603 cm−1 , with other notable features at 1398 cm−1 and 3150 cm−1 .19 Bands were observed at 1399 cm−1 and 3149 cm−1 in the spectra presented here, although there was no appreciable signal at 603 cm−1 . However, the mass spectra provide sufficient evidence of the assignment. The thermal decomposition of butyraldehyde led to the production of several species, which were identified in the FIG. 1. PIMS spectra following pyrolysis of butyraldehyde at 300 K, 1300 K, 1500 K, and 1600 K obtained with a 10.5 eV photoionization laser. Pyrolysis was performed on 0.3% samples of butyraldehyde in 2 atm of He carrier gas. matrix-isolation FTIR spectra and the PIMS spectra. Many of these were predicted from reactions (4)–(9). Others can be explained by further decomposition reactions of the initial products of butyraldehyde pyrolysis. Finally, some can best be attributed to bimolecular reactions occurring within the hyperthermal nozzle. The assignment of the various products is presented in the discussion below, which is divided into sections based on the purported reaction leading to the products being discussed. A. Products of radical decomposition Radical decomposition of butyraldehyde produces the propyl radical and HCO, which predominantly decomposes to H + CO (reaction (4)). Figure 2 shows the appearance of carbon monoxide at 2138 cm−1 .20 The CO product cannot be detected by PIMS because its ionization energy18 is 14.0 eV, above that of the photoionization laser. The propyl radical should exhibit its strongest absorption at 530 cm−1 in the FTIR spectrum,19 but there is no evidence of that feature or any of the C–H stretches. A small peak at m/z = 43 is present in the PIMS spectrum shown in Figure 1 and suggests the presence of the propyl radical (IE = 8.1 eV),21 although the signal could also be an isotopic variant of m/z = 42, where very strong PIMS signal occurs. The low PIMS signal at m/z = 43 and imperceptible FTIR absorption are likely due to secondary decomposition of the propyl radical, discussed in Sec. III G. Incidentally, the radical decomposition channel is thought to proceed by an initial C–C bond fission, producing propyl radical + HCO. The HCO radical dissociates to H + CO, although some HCO may be retained at lower temperatures or short residence times.9 The mass spectrum obtained following 1300 K pyrolysis does show evidence of HCO (IE = 8.12 eV)18 at m/z = 29, but the feature disappears at higher temperatures, indicating that a small fraction of the radicals are indeed stable at lower temperatures. The FTIR experiment was repeated with 1300 K pyrolysis, and barely perceptible bands were observed at 1861, 1093/1089, and 2488 cm−1 (not shown here), which provides FIG. 2. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-4 Hatten et al. FIG. 3. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. The symbols indicate bands that belong to unreacted butyraldehyde. at least a hint of confirmation of HCO. To be thorough, m/z = 29 also corresponds to CH3 CH2 + , and ethyl radical (IE = 8.1 eV)22 could be anticipated from reaction (8). However, there was absolutely no evidence19 in the FTIR spectra for ethyl radical, while there was (weak) spectral evidence for HCO. This is somewhat surprising, as HCO has a lower dissociation barrier and dissociation energy23 than the ethyl radical.24 B. Products of elimination The elimination reaction of butyraldehyde produces ethyl ketene and H2 (reaction (5)). Ethylketene is evidenced by bands in the FTIR spectrum at 1141 cm−1 (Figure 3), 2135 cm−1 , and 2130 cm−1 (Figure 2), matching bands observed for matrix-isolated ethylketene in the literature.25 There is also a tiny feature at m/z = 70 (CH3 CH2 CH=C=O+ ) observable in the mass spectrum following 1000 K pyrolysis. The coproduct of elimination, H2 (IE = 15.4 eV),18 cannot be observed in the mass spectra. J. Chem. Phys. 139, 214303 (2013) FIG. 4. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. The band labeled “enol” corresponds to the OH stretch of vinyl alcohol, although 1-buten-1-ol is also expected to appear in the spectrum, and would likely exhibit an OH stretch nearby. elimination of water from acetaldehyde is preceded by a ketoenol tautomerism of acetaldehyde to vinyl alcohol. If a similar mechanism governs butyraldehyde, then 1-buten-1-ol, the enol tautomer of butyraldehyde, may also be detected in these experiments. While there are no vibrational bands in the literature for matrix-isolated 1-buten-1-ol for the purpose of comparison to the FTIR spectra presented here, there is an OH stretch present at 3620 cm−1 (Figure 4) and a C=C stretch at 1663 cm−1 (Figure 5), very close to those observed in vinyl alcohol at 3619 cm−1 and 1662 cm−1 .10 However, these may very well belong to vinyl alcohol itself (vide infra), which is expected following reaction (7). Evidence of water and possibly 1-buten-1-ol in the spectra led to a search for 1-butyne, the other product of elimination in reaction (6). There is evidence at m/z = 54 for C. Products of isomerization/elimination The isomerization/elimination reaction of butyraldehyde produces 1-butyne and water (reaction (6)). Water is commonly found as a contaminant in matrix-isolation FTIR spectra as trace amounts of water vapor in the vacuum chamber can condense on the window during deposition. However, the intensity of the OH stretches and bends observed here (Figures 4 and 5) exceed what would be expected from contamination over the experimental deposition time, so it is concluded that H2 O must be a product of the pyrolysis of butyraldehyde. This was confirmed experimentally by passing pure argon through the heated pyrolysis nozzle and comparing the resultant intensities of the vibrational bands of water to those observed following the pyrolysis of butyraldehyde. The ionization energy18 of water (12.6 eV) prohibits detection via PIMS. Vasiliou and co-workers10 proposed that FIG. 5. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. The symbols indicate bands that belong to unreacted butyraldehyde. The band labeled “enol” corresponds to the C=C stretch of vinyl alcohol, although the same mode for 1-buten-1-ol would be expected in this region. This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-5 Hatten et al. FIG. 6. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. The symbols indicate bands that belong to unreacted butyraldehyde. 1-butyne (IE = 10.2 eV)18 in the PIMS spectrum (Fig. 1) obtained following 1300 K pyrolysis, albeit a diminutive peak. A recent, unpublished FTIR spectrum of 1-butyne isolated in an argon matrix measured by Ellison and co-workers26 shows that the bands of highest intensity occur at 3329 cm−1 , 1623 cm−1 , 632 cm−1 , and 626 cm−1 . The FTIR spectra measured here contain all of these bands, as well as many of the weaker bands observed in Ellison’s spectrum. Observed features of 1-butyne are labeled in Figures 2, 6, and 7. The experimental results are also consistent with the published gasphase spectrum27 which shows strong bands at 635 cm−1 , 1250 cm−1 , 2970 cm−1 , and 3320 cm−1 . The mass spectra reveal that 1-butyne disappears with increasing temperatures, suggesting that it is undergoing secondary dissociation. The thermal decomposition pathways of 1-butyne are well-established in the literature. A very low pressure pyrolysis study of 1-butyne at 1052–1152 K revealed propargyl and methyl radicals as the primary products.28 This is noteworthy because the propargyl radical is a known precursor to polycyclic aromatic hydrocarbons (PAHs) and FIG. 7. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. J. Chem. Phys. 139, 214303 (2013) FIG. 8. Matrix infrared absorption spectrum of products from the 1475 K pyrolysis of a mixture of 0.2% butyraldehyde in argon. The symbols indicate bands that belong to unreacted butyraldehyde. soot.29, 30 A shock-tube study of 1-butyne in the 1100–1600 K range resulted in the detection of methane, acetylene, ethylene, ethane, allene, propyne, C4 H2 , vinylacetylene, benzene, and 1,2- and 1,3-butadienes.31 As will be discussed in Secs. III D–III G, there is spectral evidence consistent with all of these products, except for methane, ethane, allene, benzene, and the butadienes. D. Products of the hydrogen shift/elimination reaction Reaction (7) shows the formation of ethylene and vinyl alcohol, both of which are observed in these experiments. Ethylene is clearly evidenced in the FTIR spectra at 3083 cm−1 , 1441 cm−1 , 1343 cm−1 , and 947 cm−1 (Figures 3, 7, and 8), matching literature32 values. CH2 CH2 + appears at m/z = 28 in the mass spectra shown in Figure 1. While ethylene’s ionization energy (10.5 eV)18 is very close to the energy of the ionization laser, observation of CH2 CH2 + is not unreasonable as neutral ethylene may have significant internal energy, enhancing the probability of ionization. CO+ was ruled out for the m/z = 28 peak in the mass spectra because the ionization energy of carbon monoxide18 (14.0 eV) far exceeds the energy of the ionization laser. As discussed in Sec. III C, vibrational bands observed at 3620 cm−1 (Figure 4) and 1663 cm−1 (Figure 5) are identical to those of vinyl alcohol. These bands were initially suspected as belonging to 1-buten-1-ol, but a definitive assignment of that enol cannot be made for lack of a literature comparison. The PIMS data prompted the assignment of these vibrational features to vinyl alcohol. The peak at m/z = 44 in the mass spectra could belong to CH2 CHOH+ , CH3 CHO+ , or CH3 CH2 CH3 + . However, the ionization energy of propane18 (10.9 eV) is above the photoionization laser energy, while that of vinyl alcohol22 is only 9.3 eV. The presence of acetaldehyde (CH3 CHO), the keto tautomer of vinyl alcohol, would be expected, yet attempts to identify it in the FTIR spectra were futile because many of the bands33 overlap with those of butyraldehyde. Regardless, the bands observed for vinyl alcohol perfectly matched those in the literature. Therefore, both products This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-6 Hatten et al. J. Chem. Phys. 139, 214303 (2013) of reaction (7) can be assigned in this experiment with confidence. The revelation of reaction (7) enables an interesting connection to the pyrolysis of acetaldehyde. Now that vinyl alcohol, the enol tautomer of acetaldehyde, is recognized as a product of butyraldehyde pyrolysis, it is conceivable that every product observed in the pyrolysis of acetaldehyde ought also to appear in these experiments. Vasiliou et al.9 observed the following products following the thermal decomposition of acetaldehyde: CH3 , CO, H2 C=C=O, CH2 CHOH, HC≡CH, and H2 O. Several of these products have been identified here already, and evidence for the remaining products will be presented in Secs. III E–III G. E. Possibility of β–C–C scission Reaction (8) shows the breakage of the C–C bond in the β position relative to the carbonyl of butyraldehyde, yielding ethyl and vinoxy radicals. This reaction has not been observed in the limited number of experiments concerning butyraldehyde in the literature, but it should be considered important to the mechanism because the energy of the β–C– C bond is 82.5 kcal/mol, slightly lower than the α–C–C bond (84.1 kcal/mol) that is broken in reaction (4).14 As discussed in Sec. III A, there is no strong evidence for CH3 CH2 from these experiments, but that could be explained by secondary dissociation of the ethyl radical: CH3 CH2 → CH2 CH2 + H. (10) There is some evidence suggesting the presence of the cofragment vinoxy radical, CH2 CHO, in the matrix-isolation FTIR spectra presented here. Vibrational bands are observed at 692, 723, 765, 1375, 1525, 1542, and 1558 cm−1 , matching literature19 bands. Several of these bands are quite weak or partially overlap with other bands, so the assignment is admittedly ambiguous. If vinoxy (IE = 10.2 eV)34 survives the high-temperature nozzle, it may appear at m/z = 43 in the PIMS spectra. However, observed signal at m/z = 43 was very low and could also be attributed to propyl radical, or the isotopic influence of m/z = 42. If the vinoxy has sufficient internal energy to dissociate, possible product channels are H + H2 C=C=O and CH3 + CO. The branching between these channels is dependent upon the electronic state of vinoxy. In the ground state, the H + ketene channel is suppressed and virtually all vinoxy isomerizes to acetyl, then proceeds to CH3 + CO.34, 35 This is contrary to vinoxy dissociation in the à and B̃ states, where both channels are observed and H + ketene are the major products.36, 37 Of course, the products CH3 , CO, and ketene detected in these experiments could all be attributed to other reaction pathways of butyraldehyde. While there is evidence suggesting that reaction (8) does occur, there is not absolute confidence in the assignment. F. Possibility of γ –C–C bond scission While CH3 was described in Sec. III E as a possible end result of reaction (8) via dissocation of vinoxy, it could also come directly from scission of the γ –C–C bond in butyraldehyde, shown in reaction (9). The energy for this reaction is only a few kcal/mol higher than those of reactions (5)–(8).14 The presence of CH3 , however, is not sufficient evidence for reaction (9) as there are many different sources of methyl plausible in the reaction mechanism. The cofragment, ĊH2 CH2 CHO, would almost certainly dissociate to CH2 CH2 + CO + H (which are products of other reaction channels) or to acrolein + H.35, 38 Acrolein (CH2 CHCHO) seems to be a unique product, the presence of which would lend strong support for assigning reaction (9). The FTIR spectra display bands associated with both cis- and trans-acrolein,39, 40 including 2834, 2808, 1157, 1051, 999, 917, and 905 cm−1 . Other observed bands overlap with those of unreacted butyraldehyde. Figure 3 highlights the bands that are clearly seen. Acrolein (IE = 10.1 eV)41, 42 may also be detected by PIMS (Figure 1), although m/z = 56 could also correspond to 1- or 2-butene. G. Products from secondary reactions With reasonable evidence suggesting six main decomposition pathways (reactions (4)–(9)) in butyraldehyde, this section turns to the identification of products from secondary reaction pathways. The propyl radical is a product of reaction (4), but there is only a hint of evidence for it in the mass spectrum collected following 1300 K pyrolysis, and none at higher temperatures. Propyl radical is not easily detected in these experiments because it is undergoing secondary dissociation. The propyl radical can undergo both C–C and C–H beta scission43 in the following reactions: n − C3 H7 → CH3 + CH2 =CH2 , (11) n − C3 H7 → CH3 CH=CH2 + H. (12) There is evidence for the products of both reactions (11) and (12) in the FTIR and PIMS data. CH3 + appears at m/z = 15 in Figure 1. While not all of the FTIR bands corresponding to the methyl radical were discernible, the mass spectra are convincing enough. A similar situation was encountered by Vasiliou et al. in their attempts to detect methyl radicals from the pyrolysis of acetaldehyde.9 Ethylene was already identified in Sec. III D in both matrix-isolation FTIR and PIMS experiments. While it is certainly reasonable to assume that reaction (11) is a main source of methyl radical and ethylene, it bears repeating that these products could also originate from reactions (7), (9), or (10), or decomposition of products vinoxy and 1-butyne.28, 31 Propene, likely from reaction (12), is evidenced in Figures 3 and 7 at 998 cm−1 , 909 cm−1 , and 3083 cm−1 .44 C3 H6 + appears at m/z = 42 in Figure 1, although this feature could be attributed to H2 C=C=O+ as well. While the dissociation of propyl radical is a plausible source of methyl radicals, the dissociation of 1-butyne, produced by reaction (6) in the pyrolysis of butyraldehyde, makes methyl in conjunction with the propargyl radical, CH2 C≡CH. There is evidence for the propargyl radical in these experiments at m/z = 39 (C3 H3 + ) in the mass spectra in Figure 1. This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-7 Hatten et al. The characteristic vibrational frequencies of matrix-isolated propargyl19 were not observed in the FTIR spectra presented here, but that may be a function of pyrolysis temperature. The feature at m/z = 39 is not evident following 1300 K pyrolysis, appearing only at 1500 K and 1600 K. The vibrational spectra presented here were measured following pyrolysis at a maximum temperature of 1475 K, which may have been just under the threshold needed produce sufficient propargyl for detection via FTIR. Ketene, CH2 =C=O, is evidenced by FTIR bands at 3063 cm−1 and 2142 cm−1 , and by the PIMS peak at m/z = 42. (Figures 1, 2, and 7) C2 H2 O+ and C3 H6 + overlap at m/z = 42, and both ketene and propene have ionization energies near 9.7 eV, so the infrared bands are necessary to confirm the presence of ketene. As discussed in Sec. III E, Hloss from vinoxy radical can produce ketene, although this is a suppressed channel in the ground state. Another plausible source of ketene is the secondary reaction of vinyl alcohol produced in reaction (7). Vinyl alcohol may tautomerize to acetaldehyde, which is known to produce ketene via H2 elimination under pyrolysis conditions.9 Acetylene is shown in Figures 6 and 7 at 736 cm−1 , 3302 cm−1 , and 3288 cm−1 .9 Its ionization energy is too high (11.4 eV)18 to be detected via PIMS here. There are several processes that could lead to acetylene during thermal decomposition of butyraldehyde. Elimination of H2 O from vinyl alcohol produces acetylene.9 If there is sufficient time for the vinyl alcohol from reaction (7) to react prior to deposition in the cold argon matrix, this secondary reaction could account for the presence of acetylene. Acetylene is also one of the known products of thermal decomposition of 1-butyne,31 which is produced by reaction (6). Finally, acetylene is a primary product of ethylene pyrolysis,45 and there are several reactions of butyraldehyde that lead to ethylene. As mentioned above, the thermal decomposition of 1-butyne leads to myriad chemical species. The decomposition of 1-butyne following reaction (6) may account for the detection of propyne, C4 H4 , and C4 H2 . Propyne is evidenced by FTIR bands46 at 3330, 2962, 2874, 1448, 634, 630, and 624 cm−1 in Figures 6–8. PIMS signal at m/z = 40 in Figure 1 could originate from propyne or allene, which have somewhat similar ionization energies: 10.36 eV for propyne, 9.7 eV for allene. However, there is no evidence in the FTIR spectra for allene product. C4 H4 and C4 H2 appear in the mass spectrum following pyrolysis at 1600 K exclusively. Pyrolysis was conducted at lower temperatures prior to the matrix-isolation FTIR analysis, so the vibrational modes cannot be used to identify the specific isomers of C4 H4 and C4 H2 produced. The presence of C4 H4 and C4 H2 is noteworthy, because it suggests the capacity for bimolecular carbonbuilding reactions. Isomers of C4 H4 are suspected precursors to benzene formation in certain flame conditions. Vinylacetylene can react with the vinyl radical to form benzene.47 Vinylacetylene or butatriene can react with H2 CCCCH to form aromatics via phenylacetene, pentalene, and benzocyclobutene.48 These reactions are unlikely at low temperatures but could be significant in certain combustion or pyrolysis conditions. While it is thought that reactions of J. Chem. Phys. 139, 214303 (2013) even-numbered carbon species are less likely to contribute to aromatic formation than odd-carbon species such as propargyl radical,49, 50 the presence of C4 H4 and C4 H2 suggests another route to the eventual formation of polycyclic aromatic hydrocarbons and soot in the pyrolysis of butyraldehyde. The PIMS spectrum following 1300 K pyrolysis contains signal at m/z = 56. This likely includes acrolein, as discussed in Sec. III F, but C4 H8 + was also considered as a possible product. The FTIR spectra presented here do not show signatures of 1-butene or 2-butene, likely because they were collected following 1475 K pyrolysis, and the presumed butene appears to undergo subsequent decomposition at temperatures above 1300 K. Evaluation of FTIR spectra collected following 1300 K pyrolysis (not shown here) did reveal features at 3037, 2930, 2871, 2864, 1444, 1408, and 1384 cm−1 . These bands are very close to the reported values44 for cis-2-butene, although the intensities are low and a few of the bands from the literature were not observed. H. The role of bimolecular reactions While the reactions presented in this paper reasonably explain the appearance of nearly all of the chemical species observed in the experiments and listed in Table I, the detailed mechanisms cannot be determined. What appears to be a simple unimolecular or concerted reaction, such as the elimination of H2 to form ethylketene in reaction (5), may involve bimolecular processes such as abstraction by hydrogen atoms that are liberated in reaction (4). In fact, Vasiliou and coworkers10 determined that both ketene and acetylene, shown in reactions (2) and (3), are produced by bimolecular reactions in the pyrolysis of acetaldehyde. In their work, pyrolysis of a 50:50 mixture of CH3 CHO and CD3 CDO resulted in production of H2 , D2 , and HD. The presence of HD means that a bimolecular reaction must be involved in the elimination to form ethylketene (reaction (2)). The formation of the vinyl alcohol (enol) intermediate prior to elimination in reaction (3) appears to be a unimolecular process, but Vasiliou et al. suggest that a hydrogen atom then attacks the vinyl alcohol to make CH2 CH2 OH, which dissociates to CH2 CH2 + OH. H-atom abstraction from ethylene leads to acetylene, while the OH radical can then attack other acetaldehyde molecules, abstracting a hydrogen atom to form water. In an effort to determine the molecularity of reactions (4)–(9) for butyraldehyde, the matrix-isolation FTIR experiments were repeated by carrying out pyrolysis on a 1:7000 butyraldehyde:argon mixture. Lowering the concentration of butyraldehyde should stifle, or at least severely limit, bimolecular reactions. The drawback to this approach is that it also reduces the intensity of FTIR signal. Therefore, there is some uncertainty in attributing the absence of a particular product in the FTIR to the dependence upon a bimolecular process. However, the experiments here do provide clues to the mechanisms at play. Table II shows a summary of products of various thermal decomposition reactions, whether they appear at high and low matrix ratios, and conclusions from the observations. These results indicate that reaction (4) is likely unimolecular, while reactions (5) and (6) are likely bimolecular. However, reaction (6) is attributed to a two-step process This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 206.212.5.173 On: Fri, 03 Jan 2014 17:55:29 214303-8 Hatten et al. J. Chem. Phys. 139, 214303 (2013) TABLE II. Selected products of thermal decomposition of butyraldehyde examined following pyrolysis of 1:250 and 1:7000 mixtures in argon. Checkmarks indicate the positive identification of the product via matrix-isolation FTIR. Product CH3 CH=CH2 CH2 =CH2 CH3 CH2 CH=C=O CH3 CH2 C≡CH CH2 =CHOH Reaction(s) of origin 1:250 1:7000 Conclusions/notes 12 (via 4) 7, 10 (via 8), or 11 (via 4) 5 6 7 Reactions (4) and (12) are likely unimolecular. At least one of reactions (7) and (10), and (11) is unimolecular. Reaction (5) is likely bimolecular. Reaction (6) is likely bimolecular, with the caveat that it could proceed via an enol intermediate. Either step could be bimolecular. Reaction (7) may be bimolecular. (keto-enol tautomerism followed by H2 O elimination) and it is impossible to speculate on the molecularity of each step without the ability to assign definitively the 1-buten-1-ol intermediate. Reaction (7) is ambiguous, but may be bimolecular. This would be surprising, as it has previously been suggested to be a unimolecular elimination.11 Further study of this reaction may be worthwhile. A survey of the list of products in Table I also hints at the existence of bimolecular reactions. For example, propane is evidenced51 by FTIR in Figures 3, 6, and 8, but not PIMS, due to its 10.9 eV ionization energy.18 It is difficult to conceive a unimolecular path from butyraldehyde to propane. The combination of propyl radical and a hydrogen atom seems more plausible. Similarly, the presence of products C4 H2 and C4 H4 cannot easily be explained by unimolecular processes. If these products originate from the decomposition of 1-butyne, as observed in a published shock tube study,31 then bimolecular reactions are certainly involved. It is also conceivable that reactions of acetylene could lead to these products via a mechanism that must include bimolecular reactions.52 IV. CONCLUSIONS The thermal decomposition of gas-phase butyraldehyde in argon has been studied in the 1300–1600 K range with a hyperthermal nozzle. The products detected via matrixisolation FTIR and/or PIMS were: CO, HCO, CH3 CH2 CH2 , CH3 CH2 CH=C=O, H2 O, CH3 CH2 C≡CH, CH2 CH2 , CH2 =CHOH, CH2 CHO, CH3 , HC≡CH, CH2 CCH, CH3 C≡CH, CH3 CH=CH2 , H2 C=C=O, CH3 CH2 CH3 , C4 H2 , C4 H4 , CH2 =CHCHO, and C4 H8 . At least six initial reactions are associated with the thermal decomposition mechanism, plus numerous subsequent reactions. Several of the reactions appear to be bimolecular in nature. The presence of propargyl radical, C4 H2 , and C4 H4 suggests that the thermal decomposition of butyraldehyde could lead to formation of polycyclic aromatic hydrocarbons, an important consideration when evaluating the sooting potential of industrial processes where aldehydes are exposed to high temperatures. It is of note that these experiments are qualitative in that they identify the products of butyraldehyde pyrolysis. This paper’s comprehensive picture of the products of pyrolysis combined with the consideration of possible reactions at play in the mechanism should provide a natural stepping stone to future studies modeling the kinetics and establishing an overall mechanism for pyrolysis. ACKNOWLEDGMENTS This work was supported by an award from Research Corporation for Science Advancement and a Faculty Startup Award from The Camille and Henry Dreyfus Foundation. This material is also based upon work supported by MUADVANCE via the National Science Foundation under Grant Nos. 0548113 and 0929997. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation. C.D.H. acknowledges a fellowship from the SURE Program funded through the West Virginia Research Challenge Fund, and administered by the West Virginia Higher Education Policy Commission, Division of Science and Research, Grant No. HEPC.dsr.11.24; AMEND 1. The authors thank Barney Ellison, Jong Hyun Kim, and Jessie Porterfield for technical assistance in collecting the mass spectra presented in this paper. 1 C. Lievens, D. Mourant, M. He, R. Gunawan, X. Li, and C.-Z. Li, Fuel 90, 3417 (2011). 2 C. Tessini, N. Mueller, C. Mardones, D. Meier, A. Berg, and D. von Baer, J. Chromatogr. A 1219, 154 (2012). 3 R. R. Baker and L. J. Bishop, J. Anal. Appl. 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