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Research Article Received: 4 October 2013, Revised: 5 December 2013, Accepted: 18 December 2013, Published online in Wiley Online Library: 5 February 2014 (wileyonlinelibrary.com) DOI: 10.1002/poc.3282 Kinetics and mechanisms of gas-phase decarbonylation of α-methyl-transcinamaldehyde and E-2-methyl-2-pentenal under homogeneous catalysis of hydrogen chloride Libia L. Julioa, Jesus Lezamaa, Alexis Maldonadoa, José R. Moraa and Gabriel Chuchania* The kinetics of the gas-phase elimination of α-methyl-trans-cinamaldehyde catalyzed by HCl in the temperature range of 399.0–438.7 °C, and the pressure range of 38–165 Torr is a homogeneous, molecular, pseudo first-order process and undergoing a parallel reaction to produce via (A) α-methylstyrene and CO gas and via (B) β-methylstyrene and CO gas. The decomposition of substrate E-2-methyl-2-pentenal was performed in the temperature range of 370.0–410.0 °C and the pressure range of 44–150 Torr also undergoing a molecular, pseudo first-order reaction gives E-2-pentene and CO gas. These reactions were carried out in a static system seasoned reactions vessels and in the presence of toluene free radical inhibitor. The rate coefficients are given by the following Arrhenius expressions: Products formation from α-methyl-trans-cinamaldehyde  α-methylstyrene: logk′1 s 1 lmol 1 ¼ ð12:67±0:02Þ ð183:3±0:31ÞkJmol 1 ð2:303RT Þ β-methylstyrene:logk ′1 s 1 lmol 1 ¼ ð13:19±0:03Þ ð183:0±0:45ÞkJmol 1 ð2:303RT Þ Products formation from E-2-methyl-2-pentenal  E-2-pentene: logk ′1 s 1 lmol 1 ¼ ð12:79±0:06Þ ð174:5±0:80ÞkJmol 1 ð2:303RT Þ 1 1 1 The kinetic and thermodynamic parameters for the thermal decomposition of α-methyl-trans-cinamaldehyde suggest that via (A) proceeds through a bicyclic transition state type of mechanism to yield α-methylstyrene and carbon monoxide, whereas via (B) through a five-membered cyclic transition state to give β-methylstyrene and carbon monoxide. However, the elimination of E-2-methyl-2-pentenal occurs by way of a concerted cyclic five-membered transition state mechanism producing E-2-pentene and carbon monoxide. The present results support that uncatalyzed α-β-unsaturated aldehydes decarbonylate through a three-membered cyclic transition state type of mechanism. Copyright © 2014 John Wiley & Sons, Ltd. Keywords: kinetics; gas-phase elimination; α-methyl-trans-cinamaldehyde; E-2-methyl-2-pentenal INTRODUCTION 450 Aldehydes are organic molecules difficult to study in homogeneous, unimolecular gas-phase thermal decomposition kinetics in the gas phase. This type of compounds are liable to be oxidized in the presence of oxigene and to undergo a complex free radical reactions.[1] In this sense, the thermal decomposition of low molecular saturated aldehydes, formaldehyde,[2–4] acetaldehyde,[5–20] propionaldehyde,[21–27] and at temperatures above 450 °C, have shown to undergo complex free radical processes. However, the aromatic aldehyde, benzaldehyde[28–32] at 550–1400°C decomposed via a radical reaction yielding benzene and CO gas, and small amounts of biphenyl and hydrogen gas. 2,2-Dimethyl-3-butenal, the only β-γ-unsaturated aldehyde, studied in gas-phase kinetic decomposition[33] (282–302 °C), was found to produce 2-methyl-2-butene and carbon monoxide. The kinetic isotope effect of this reaction gave a kH/kD = 2.8 at 296.9 °C (i.e., 7.2 at 25 °C), suggesting that the aldehyde J. Phys. Org. Chem. 2014, 27 450–455 hydrogen migrated during the slow step of the reaction. These results imply a unimolecular reaction and obeying a first-order rate law, thus suggesting a five-membered cyclic transition state type of mechanism as described in reaction (1). (1) * Correspondence to: Gabriel Chuchani, Centro de Química, Instituto Venezolano de Investigaciones Científicas, Apartado 21827, Caracas, Venezuela. E-mail: chuchani@ivic.gob.ve a L. L. Julio, J. Lezama, A. Maldonado, J. R. Mora, G. Chuchani Centro de Química, Instituto Venezolano de Investigaciones Científicas, Apartado, 21827, Caracas, Venezuela Copyright © 2014 John Wiley & Sons, Ltd. GAS-PHASE DECOMPOSITION OF UNSATURATED ALDEHYDES CATALYZED BY HCL Grela and Colussi[32], besides reporting the pyrolysis kinetic of benzaldehyde in a flow system, included in the work the thermal decomposition of 2-furaldehyde and 2-butenal. The 2furaldehyde gave a biradical mechanism, whereas 2-butenal proved to be a molecular process. The evaluation of the mechanism of 2-butenal was performed by a copyrolysis of 2butenal in a 1:3 mixture of normal and 2-butenal-O-d, where it was found a nearly the same ratio in the products C3H5D and C3H6, with a negligible kinetic isotope effect of 0.97 ± 0.1. Based from this result, it was proposed the mechanism of 2-butenal to proceed through a tight concerted three-membered cyclic transition state structure with an A factor of 1013.5 s 1 as depicted in reaction (2). (2) Chuchani and collaborators[34] studied the gas-phase thermal decarbonylation of two α-β-unsaturated aldehydes: E-2-butenal and E-3-phenyl-methylpropenal. The kinetics was determined in a static reaction system at the temperature range of 430– 480 °C (703.15–753.15 K). These reactions showed to be homogeneous, unimolecular, and followed a first-order law. The decomposition products of 2-butenal are propene and CO gas, whereas 3-phenyl-2-methylpropenal yielded α-methylstyrene, cis-trans-β-methylstyrene, indan, and CO gas. The reported kinetics and thermodynamics data suggested these elimination reactions to proceed through a three-membered cyclic transition state type of mechanisms, thus supporting the proposal of Grela and Colussi[32] for α-β-unsaturated aldehydes decomposition. However, a two-steps mechanism for the formation of a carbene type of intermediate through a four-membered cyclic transition structure was not contemplated. The proposed three-membered cyclic transition state type of mechanism from few works in gas-phase thermal decomposition of α-β-unsaturated aldehydes appears to require verification or support of this type of transition state by using a catalysis such as hydrogen chloride. In this respect, undertaking an experimental task of decarbonylation of α-β-unsaturated aldehydes by incorporating the effect of a catalyst such as HCl gas under homogeneous conditions is a challenge. Consequently, the present work aimed at examining the gas-phase elimination kinetics of α-methyl-trans-cinamaldehyde and E-2-methyl-2-pentenal catalyzed by HCl gas. EXPERIMENTAL SECTION J. Phys. Org. Chem. 2014, 27 450–455 The thermal decomposition experiments were performed in cylindrical vessels seasoned or deactivated by the products of decomposition of allyl bromide in a static system,[35–37] and the rate coefficients were determined manometrically (mercury manometer). The temperature was controlled within ±0.2 °C with a SHINKO DIC-PS (Shinko, Senbahigashi, Osaka, Japan) 23TR resistance thermometer controller with a calibrated Iron Constantan thermocouple. The temperature reading was measured within ± 0.1 °C with the Iron-Constantan thermocouple attached to a Digital Multimeter Omega 3465B. The reaction vessel showed no temperature gradient at different points, and the substrates were injected directly into the reaction vessel through a silicone rubber septum. HCl gas was added into the reaction vessel to an amount measured manometrically from a reservoir of the system. The volume of substrate used for each reaction was ≈0.05–0.1 ml. RESULTS AND DISCUSSION The elimination reaction of α-methyl-trans-cinamaldehyde and E-2-methyl-2-pentenal catalyzed by HCl gas, in a static deactivated reaction vessel with allyl bromide decomposition and in the presence of toluene free radical suppressor, produces CO gas and the corresponding olefin as described in reaction (3) and (4): (3) (4) The experimental stoichiometry for reactions (3) and (4) was checked by carrying out the decomposition process until no further pressure increase was observed. These stoichiometries for product formations requires that, for long reaction times, Pf = 2 P0, where Pf and P0 are the final and initial pressure, respectively. The average experimental results for Pf/P0 values at five different temperatures and 10 half-lives were 1.95 for α-methyl-transcinamaldehyde and 1.90 for E-2-methyl-2-pentenal (Table 1). The stoichiometries of (3) and (4) are shown in Table 2. For both unsaturated aldehydes, up to about 40% reaction, there is a reasonable agreement between the extents of decomposition of the substrate as predicted from pressure measurements and form the chromatographic analyses of products formation. Product distributions in the thermal decomposition of αmethyl-trans-cinamaldehyde as described in reaction (3) at 40% reaction at 420 °C and at different temperatures are specified in Tables 3 and 4. The quantitative chromatographic analysis of the styrene products indicates a kinetic control in the process of elimination. The ratio %β-methylstyrene/%α-methylstyrene shows a ratio kβ/kα of 3.54 in the temperature range, where βmethylstyrene is favored by the kinetic control and the more thermodynamic stable isomer. Copyright © 2014 John Wiley & Sons, Ltd. wileyonlinelibrary.com/journal/poc 451 The starting materials α-methyl-trans-cinamaldehyde (99.1%) and E-2methyl-2-pentenal (98.0%) were acquired from Aldrich. The purity of the substrates and products were determined by GC/MS/MS (Saturn 2000, Varian). Capillary column DB – 5MS, 30 × 0.250 mm. id. 0.25 μm. The quantitative chromatographic analyses of α-methylstyrene, βmethylstyrene, and E-2-pentene were determined by using a gas chromatograph Hewlett Packard 5710-A with a Chromosorb 103, 80–100 mesh 1 m and internal diameter of 2 mm. The identification of the products was made by comparing chromatogram of the reaction products with true authentic samples bought from Aldrich and in a GC–MS (Saturn 2000, Varian 3600X with a DB-5MS capillary column 30 × 0.25 mm. i.d. and 0.25 μm). Kinetics L. L. JULIO ET AL. Table 1. Ratio of final (Pf) to initial pressure (P0)a Table 4. Olefin distribution at different temperatures of αmethyl-trans – cinamaldehyde at 35% decomposition α-methyl-trans-cinamaldehyde P0(Torr) Pf(Torr) Pf/P0 Average 53 65 47 48 84 104 124 92 95 165 1.96 1.91 1.97 1.97 1.96 1.95 ± 0.02 E-2-methyl-2- pentenal 371.1 64 380.7 60 390.6 59 399.6 74 409.3 76 121 113 111 140 149 1.90 1.88 1.88 1.89 1.96 1.90 ± 0.03 Temperature 399.2 410.2 421.0 430.0 437.4 Temperature (°C) % α-Methylstyrene % β-Methylstyrene 22.2 22.0 21.9 77.8 78.0 78.1 410.0 420.0 430.0 Seasoned vessel with presence of twofold toluene inhibitor and threefold of HCl gas with respect to the substrate. a Seasoned vessel with presence of toluene inhibitor of ≈2P0 and threefold of HCl gas with respect to the substrate. significant effect on the rates. However, when the packed and unpacked vessels are seasoned or deactivated with allyl bromide decomposition products, no effect on the rate coefficients was obtained (Table 5). These results suggest that the polymeric layer formed in the thermal decomposition of allyl bromide does not affect the rate coefficient, and consequently, the homogeneity is confirmed. Table 5. Homogeneity of the reaction Table 2. Stoichiometry of the reactions Substrate a S/V (cm 1) Temperature Time % % Reaction (°C) (min) Productb (pressure) (GC) α-methyl-transcinamaldehyde 420.0 °C E-2-methyl-2pentenal 390.7 ° C 4 5 7 10 4 6 10 15 7.8 12.7 22.5 36.1 14.3 21.3 32.0 42.9 8.0 13.5 23.7 37.0 13.0 20.0 31.0 43.0 a Seasoned vessel with presence of twofold toluene inhibitor, and threefold of HCl gas with respect to the substrate. b These values are the total percentage of products. 106 k1(Torr 1 s 1)(a) 106 k1(Torr 1 s 1)(b) α-Methyl-trans-cinamaldehyde at 420.0 °C 1.0 9.90 ± 5.30 6.0 12.80 ± 7.00 7.80 ± 0.23 7.84 ± 0.10 E-2-methyl-2-pentenal at 391.7 °C 1.0 7.56 ± 4.50 6.0 9.70 ± 8.70 2.85 ± 0.97 2.88 ± 1.90 S, surface; V, volume. Presence of twofold toluene inhibitor, and threefold of HCl gas with respect to the substrate a Clean Pyrex vessel. b Vessel deactivated with allyl bromide. Table 6. Effect of toluene inhibitor on rates Table 3. Olefin distribution of α-methyl-trans-cinamaldehyde decomposition at different % reaction. Time (min) 4 5 7 10 % Reaction % α-Methylstyrene % β-Methylstyrene 7.8 12.7 22.5 37.0 22.1 22.0 21.8 22.0 77.9 78.0 78.2 78.0 Temperature 420.0 °C. Seasoned vessel with presence of twofold toluene inhibitor and threefold of HCl gas with respect to the substrate. 452 The homogeneity of these elimination reactions, in the presence of the chain inhibitor toluene, was examined by carrying out several runs in a vessel with a surface-to-volume ratio of about 6.0 relative to that of the normal vessel, which is equal to one. The packed and unpacked clean Pyrex vessel gave a wileyonlinelibrary.com/journal/poc P0 (Torr) Pi (Torr) Pi/P0 106 k1 (Torr 1 s 1) k1 (cm3mol 1 s 1) α-Methyl-trans-cinamaldehyde at 420.0 °C 61 — — 6.90 ± 0.20 55 56 1.02 7.40 ± 0.01 41 60 1.46 7.79 ± 0.01 46 92 2.00 7.79 ± 0.36 27 62 2.30 7.80 ± 0.20 298.53 ± 8.65 320.16 ± 0.43 337.20 ± 0.43 337.10 ± 15.57 337.46 ± 8.65 E-2-methyl-2-pentenal at 389.7 °C 47 — — 2.64 ± 0.07 73 85 1.16 2.76 ± 0.05 74 112 1.51 2.87 ± 0.06 56 114 2.04 2.87 ± 0.10 50 120 2.40 2.87 ± 0.10 109.19 ± 2.89 114.16 ± 2.06 118.70 ± 2.50 118.50 ± 4.13 118.20 ± 4.13 P0, pressure of the substrate; Pi, pressure of the inhibitor toluene inhibitor of ≈2P0. Vessel deactivated with allyl bromide. Presence of threefold of HCl gas with respect to the substrate. Copyright © 2014 John Wiley & Sons, Ltd. J. Phys. Org. Chem. 2014, 27 450–455 504.88 ± 1.32 508.00 ± 0.88 507.07 ± 2.19 509.70 ± 2.63 42.50 ± 1.61 41.40 ± 1.21 43.41 ± 4.02 42.50 ± 0.80 J. Phys. Org. Chem. 2014, 27 450–455 Copyright © 2014 John Wiley & Sons, Ltd. 410.0 6.73 ± 0.14 287.00 ± 5.97 s 1) 1 s 1) Rate equation: log k1(s 1Lmol 1) = (13.19 ± 0.03) (183.0 ± 0.45) kJmol 1(2.303RT) 1 r = 0.9998 370.0 380.7 390.7 399.6 1.06 ± 0.02 1.77 ± 0.06 2.87 ± 0.08 4.25 ± 0.15 42.50 ± 0.80 72.50 ± 2.44 118.70 ± 3,31 178.50 ± 6.30 Rate equation: log k1(s 1Lmol 1) = (12.79 ± 0.06) (174.5 ± 0.80) kJmol 1(2.303RT) 1 r = 0.9997 438.7 13.1 ± 0.02 581.00 ± 0.88 wileyonlinelibrary.com/journal/poc 453 Seasoned vessel with presence of twofold of toluene inhibitor and threefold of HCl gas with respect to the substrate 1 s 1) Temp. (°C) 106 k1(Torr k1(cm3mol E-2-methyl-2-pentenal at 371.1 °C 65 1.05 ± 0.04 61 1.03 ± 0.03 57 1.08 ± 0.10 44 1.06 ± 0.02 1 E-2-pentene α-Methyl-trans-cinamaldehyde at 429.8 °C 60 11.51 ± 0.03 57 11.58 ± 0.02 48 11.56 ± 0.05 46 11.62 ± 0.06 k1(cm3mol s 1) 1 s 1) s 1) 1 1 Temp. (°C) 106 k1(Torr k1(cm3mol 106 k1(Torr β-methyl styrene Table 8. Invariability of rate coefficient with initial pressure of the substrate P0(Torr) Rate equation: log k1(s 1Lmol 1) = (12.67 ± 0.02) (183.3 ± 0.31) kJmol 1(2.303RT) 1 r = 0.9998 399.1 408.9 421.0 430.0 2.23 ± 0.02 3.53 ± 0.04 6.06 ± 0.08 9.02 ± 0.03 93.54 ± 0.83 150.23 ± 1.70 262.50 ± 3.50 395.94 ± 1.31 Seasoned vessel with presence of twofold of toluene inhibitor. P0 substrate ≈ 45.0 Torr 399.1 0.63 ± 0.01 26.38 ± 0.41 2.85 ± 0.03 2.88 ± 0.02 2.85 ± 0.05 2.88 ± 0.03 2.86 ± 0.04 s 1) 1 s 1) E-2-methyl-2-pentenal at 390.5 °C 249 7.10 ± 0.07 229 6.60 ± 0.05 207 5.90 ± 0.10 191 5.50 ± 0.05 175 5.00 ± 0.07 1 7.76 ± 0.31 7.82 ± 0.27 7.80 ± 0.40 7.76 ± 0.35 7.70 ± 0.11 Temp. (°C) 106 k1(Torr k1(cm3mol α-Methyl-trans-cinamaldehyde at 420.2 °C 219 17.00 ± 0.70 110 8.60 ± 0.30 100 7.80 ± 0.40 85 6.60 ± 0.30 74 5.70 ± 0.85 408.9 0.99 ± 0.01 42.38 ± 0.42 s 1) α-methyl styrene 1 Parameters 106 k1(Torr Product 104kobs(s 1) Table 9. The variation of the rate coefficients with temperatures PHCl(Torr) 438.7 3.69 ± 0.01 163.86 ± 0.44 Table 7. Effect of HCl gas catalyst on the rate of decarbonylation 421.0 1.71 ± 0.02 74.11 ± 0.86 Values The kinetic runs of these substrates were performed in the presence of at least twice the amount of the radical chain suppressor toluene in order to inhibit any possible radical chain reactions. The effect of different proportions of toluene in the process is shown in Table 6. The absence of toluene inhibitor yields a small decrease in the rate coefficient with values of 6.90 × 10 6 (Torr 1 s 1) and 2.64 × 10 6 (Torr 1 s 1) for α-methyl-trans-cinamaldehyde and E-2-methyl-2-pentenal elimination, respectively. When the reaction is carried out in the presence of toluene in ratios Pi/P0 from 1.0 to 2.6, the rate coefficient is constant, and any radical chain reaction is suppressed. In the pseudo first-order rate law described in Equation (1), the rate coefficient kobs is not independent of the catalyst HCl pressure, which indicates that the variation of PHCl gives different values of kobs-values. Therefore, the second-order rate coefficient is obtained by dividing kobs into PHCl. Thus, Equation (1) changes into Equation (2). In Table 7 are shown the values of the kobs with different values of PHCl from 74 to 249 Torr 430.0 2.55 ± 0.01 111.66 ± 0.43 GAS-PHASE DECOMPOSITION OF UNSATURATED ALDEHYDES CATALYZED BY HCL L. L. JULIO ET AL. obtained by the fitting of PT = P0[2-exp( kobst)] by using OriginPro 8.0 program (Origin Lab Co., Northhampton, MA, USA), and it was observed a constant value in the second-order rate constant in agreement with the predicted by the Equation (2). kobs ¼ PHCI k1 ¼ ð1=tÞ ln k1 ¼ ð1=tÞð1=PHCI Þ ln P0 ð2P0 PT Þ P0 ð2P0 PT Þ (1) (2) The rate coefficient of these decarbonylation reactions, at constant HCl gas pressure, was found to be independent of the initial pressures (Table 8). The second-order rate coefficient was estimated from Equation (2). To propose an elimination mechanism and discuss the observed difference in the reactivity of these two compounds (Tables 6–8), it was considered the variation of the rate coefficients with temperatures. For the decomposition of α-methyltrans-cinamaldehyde (PHCl/P0 = 3.7) and E-2-methyl-2-pentenal (PHCl/P0 = 4.0), the results are given in Table 9. This table leads, by using the least-squares procedure and 90% confidence limits, to obtain the Arrhenius equations of each reaction. According to the results of Table 9, the activation energy for the formation of α-methyl styrene and β-methyl styrene is similar (183.0 kJmol 1), yet the isomer β-methyl styrene is kinetically favored because log A value is greater than the value of the αmethyl styrene formation. Therefore, these parallel reactions proceed through different transition states. The activation energy of E-2-methyl-2-pentenal decomposition was 174.5 kJmol 1, which is a lower value when compared with that obtained for the elimination of α-methyl-trans-cinamaldehyde. Combining the Arrhenius expression with the Eyring equation, it is possible to obtain the thermodynamic parameters of activation as ∆S‡, ∆H‡, and ∆G‡. In Table 10, the kinetic and thermodynamic activation parameters for the elimination process studied in the present work are listed. The kinetic and thermodynamic parameters of Table 10 reveal the homogeneous molecular nature of the gas-phase thermal decomposition of α-methyl-trans-cinamaldehyde and E-2-methyl2-pentenal catalyzed by HCl gas. According to products formation of α-methyl-trans-cinamaldehyde, a parallel elimination takes place. Via A proceeds through a concerted bicyclic transition state type of mechanism (∆S≠ = 25.5 Jmol 1 K 1). In this respect, the polarization of the Cδ –Hδ+ bond of the CHO group is the limiting factor. This way a phenyl group may undergo through an intramolecular Wagner–Meerwein type of rearrangement. Because of this, the partial positive charge at the Cα atom is then stabilized (reaction 5 (via A)). In the case of the decomposition through via B, the formation of β-methyl styrene and CO gas appears to be the result of a concerted five-membered cyclic transition state type of mechanism (reaction 5 (via B)). As previously described, these two parallel reactions proceed through different transition states and therefore distinct values in the activation entropy. This difference in rate coefficients of these two parallel processes is dominated by the entropic effects. The α-methyl styrene (Table 10) shows log A = 12.67 and a more negative value in activation entropy of 25.5 Jmol 1 K 1. This transition state is more rigid and presents a major lost in translational, rotational and vibrational degrees of freedom when compared with the transition state involved in the β-methyl styrene formation. With regard to E-2-methyl-2-pentenal elimination reaction, the formation of E-2-pentene implies a mechanism similar to the process of β-methyl styrene formation from the α-methyl-transcinamaldehyde (reaction 5, via B). This means a concerted fivemembered cyclic transition state (reaction 6). When via B of αmethyl-trans-cinamaldehyde elimination (β-methyl styrene formation) is compared with that of E-2-methyl-2-pentenal, a small difference in the activation enthalpy is found. This difference is due to the stabilization of the partial negative carbon atom formed in the rate determining factor Cδ –Hδ+. This fact infers an impediment for electron delocalization in the transition state due to the steric interaction between the methyl group and the aromatic nuclei (reaction 5). Hence, the sequence in rates is E-2-methyl-2-pentenal > α-methyl-trans-cinamaldehyde. (5) (6) Table 10. Kinetic and thermodynamic activation parameters at 410.0 °C (683.15 K) Product log A Ea (kJmol 1) ∆S‡ (Jmol 1 K 1) ∆H‡ (kJmol 1) ∆G‡ (kJmol 1) 454 α-methyl-trans-cinamaldehyde β-methyl styrene 13.19 ± 0.03 α-methyl styrene 12.67 ± 0.02 183.0 ± 0.31 183.3 ± 0.45 15.4 25.5 172.3 172.6 182.2 189.0 E-2-methyl-2-pentenal E-2-pentene 174.5 ± 0.80 23.1 163.7 178.6 12.79 ± 0.06 wileyonlinelibrary.com/journal/poc Copyright © 2014 John Wiley & Sons, Ltd. J. Phys. Org. Chem. 2014, 27 450–455 GAS-PHASE DECOMPOSITION OF UNSATURATED ALDEHYDES CATALYZED BY HCL The consideration of these mechanisms (reactions 5 and 6) insinuates that uncatalyzed α-β-unsaturated aldehydes may well decarbonylate through a three-membered cyclic transition state type of mechanism. Consequently, the present results appear to support the mechanisms of thermal decomposition of α-β-unsaturated aldehydes in the gas phase reported in the literature.[32,34] [15] [16] [17] [18] [19] [20] [21] [22] REFERENCES [23] [1] F. A. Carey, R. J. Sundberg, Advanced Organic Chemistry. Part A: Structure and Mechanism, 4th Edition. Kluwer Academic/Plenum Publishers, New York, 2000, p. 202. [2] R. Klein, M. D. Scheer, L. J. Schoen, J. Am. Chem. Soc. 1956, 78, 50. [3] H. G. Schecker, W. Jost, Ber. Bunsenges. Phys. Chem. 1969, 73, 521. [4] C. J. Chen, D. J. McKenney, Can. J. Chem. 1972, 50, 992. [5] L. S. Kassel, J. Phys. Chem. 1930, 34, 1166. [6] C. J. M. Fletcher, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1933, 141, 41. [7] F. O. Rice, K. F. Herzfeld, J. Am. Chem. Soc. 1934, 56, 284. [8] C. A. Winkler, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1935, 149, 355. [9] E. Leifer, H. C. Urey, J. Am. Chem. Soc. 1942, 64, 994. [10] J. R. Freeman, J. C. Danby, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1958, 245, 456. [11] S. K. Ho, Proc. Roy. Soc. Lond. Ser. A 1963, 276, 278. [12] A. B. Trenwith, J. Chem. Soc. 1963, 4426. [13] R. W. Dexter, A. B. Trenwith, J. Chem. Soc. 1964, 5459. [14] M. Eusuf, K. J. Laidler, Can. J. Chem. 1964, 42, 1851. [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] [35] [36] [37] N. Imai, O. Toyama, Bull. Chem. Soc. Japan. 1967, 40, 81. K. J. Laidler, M. T. H. Lui, Proc. Roy. Soc. Lond. Ser. A, 1967, 297, 365. M. T. H. Liu, Can. J. Chem. 1968, 46, 479. I. Bardi, F. Márta, Acta Phys. Chem. 1973, 19, 227 I. Bardi, F. Márta, Acta Phys. Chem. 1974, 20, 47. P. F. Knewstubb, J. Chem. Soc. Faraday Trans. 2 1989, 85, 671. C. N. Hinshelwood, H. W. Thompsom, Proc. Roy. Soc. Lond. Ser. A 1926, 113, 221. C. A. Winkler, C. J. M. Fletcher, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A 1934, 146, 345. J. R. E. Smith, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1942, 180, 237. T. J. Sworski, M. Burton, J. Am. Chem. Soc. 1951, 73, 3194. Z. G. Szabó, F. Márta, J. Am. Chem. Soc. 1961, 83, 768. D. H. Volman, R. K. Brinton, J. Chem. Phys. 1954, 22, 929. K. J. Laidler, M. Eusuf, Can. J. Chem. 1965, 43, 268. R. E. Smith, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1940, 175, 131. R. E. Smith, C. N. Hinshelwood, Proc. Roy. Soc. Lond. Ser. A, 1942, 180, 253. K. U. Ingold, F. P. Lossing, Can. J. Chem. 1953, 31, 30. R. E. Smith, Trans. Faraday Soc. 2 1940, 36, 983. M. A. Grela, A. J. Colussi, J. Phys. Chem. 1986, 90, 434. R. J. Crawford, S. Lutener, H. Tokunaga, Can. J. Chem. 1977, 55, 3951 O. Y. Chabán, R. M. Domínguez, A. Herize, M. Tosta, A. Cuenca, G. Chuchani, J. Phys. Org. Chem. 2007, 20, 307. A. Maccoll, J. Chem. Soc. 1955, 965. E. S. Swinbourne, Aust. J. Chem. 1958, 11, 314. R. M. Dominguez, A. Herize, A. Rotinov, A. Alvarez-Aular, G. Visbal, G. Chuchani, J. Phys. Org. Chem. 2004, 17, 399. 455 J. Phys. Org. Chem. 2014, 27 450–455 Copyright © 2014 John Wiley & Sons, Ltd. wileyonlinelibrary.com/journal/poc