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Download Free PDFKinetics and thermochemistry of the hydroxycyclohexadienyl radical reaction with O2: C6H6OH + O2 ? C6H6(OH)OO
Lev Krasnoperov2004, The Journal of Physical Chemistry a
https://doi.org/10.1021/JP030935Cvisibility…
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The UV absorption spectrum along with the self-reaction and oxidation reaction kinetics of the hydroxycyclohexadienyl radical, C 6 H 6 OH (which results from OH addition to benzene), were studied using excimer laser photolysis coupled to transient UV absorption. The radicals were generated by photolysis of N 2 O/H 2 O/ C 6 H 6 /He mixtures at 193 nm in a series of chemical reactions initiated by O( 1 D). The radical has continuous absorption in the range 260-340 nm with a maximum absorption cross-section of (8.1 ( 1.4) × 10 -18 cm 2 molecule -1 at 280 nm. Reaction of the radical with molecular oxygen, C 6 H 6 OH + O 2 h C 6 H 6 (OH)OO (1), and self-reaction C 6 H 6 OH + C 6 H 6 OH f products (2), were studied over the 252-285 K temperature range at 1.01 ( 0.02 bar (He). The radical temporal profiles were recorded via transient absorption at 315 nm. In reaction 1, two-time-domain "equilibration" kinetics were recorded in the temperature range 252-273 K. The rate constant of the addition reaction is k 1 ) (1.4 ( 0.8) × 10 -12 exp(-18.6 ( 1.7 kJ mol -1 /RT) cm 3 molecule -1 s -1 . The standard enthalpy of reaction 1 was determined from the measured equilibrium constants using the third law method: ∆H°2 98 ) -43.6 ( 2.0 kJ mol -1 . The measured rate constant of self-reaction 2 is k 2 ) (6 ( 3) × 10 -11 exp(-2.00 ( 1.6 kJ mol -1 /RT) cm 3 molecule -1 s -1 .
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We have used laser-photolysis/photoionization mass spectrometry to measure the kinetics of the reaction of 1-methylpropargyl (but-3-yn-2-yl, CH = C −CH-CH 3) radicals with oxygen molecules as a function of temperature (T = 200 − 685 K) and bath gas density (1. 2 − 15 × 10 16 cm −3). The low temperature (T ≤ 304 K) kinetics is dominated by oxygen addition to the −CHcarbon of the radical to form a peroxyl radical, and the measured CH = C −CH-CH 3 + O 2 bimolecular rate coefficient exhibits negative temperature dependence and depends on bath gas density. At slightly higher temperatures (335 − 396 K), where the redissociation rate of the peroxyl is already observable, we measured the CH = C = CH-CH 3 + O 2 − − − − CH ≡C-C (OO •)H-CH 3 equilibrium constant as a function of temperature. At even higher temperatures (T = 479 − 685 K), the loss rate of 1-methylpropargyl is determined by the addition of oxygen to the terminal H-C = carbon and the reaction is observed to produce methylketene. The high-temperature CH = C −CH-CH 3 + O 2 bimolecular rate coefficient is independent of bath gas density and the temperature dependence is weakly positive. To explain our experimental findings, we performed quantum chemical calculations together with master equation simulations. By using our experimental data to constrain key parameters, the master equation model was able to reproduce experimental results reasonably well. We then extended the conditions of our simulations up to 2000 K and 100 bar. The results of these simulations are provided in ChemKin compatible PLOG format.
downloadDownload free PDFView PDFchevron_rightKinetics and thermochemistry of the reaction of 3-methylpropargyl radical with molecular oxygenRaimo TimonenProceedings of the Combustion Institute, 2019
We have measured the kinetics and thermochemistry of the reaction of 3-methylpropargyl radical (but-2-yn-1-yl) with molecular oxygen over temperature (223 − 681 K) and bath gas density (1.2 − 15.0 × 10 16 cm −3) ranges employing photoionization mass-spectrometry. At low temperatures (223 − 304 K), the reaction proceeds overwhelmingly by a simple addition reaction to the −CH 2 end of the radical, and the measured CH 3 CCCH • 2 + O 2 reaction rate coefficient shows negative temperature dependence and depends on bath gas density. At intermediate temperatures (340−395 K), the addition reaction equilibrates and the equilibrium constant was determined at different temperatures. At high temperatures (465 − 681 K), the kinetics is governed by O 2 addition to the third carbon atom of the radical, and rate coefficient measurements were again possible. The high temperature CH 3 CCCH • 2 + O 2 rate coefficient is much smaller than at low T , shows positive temperature dependence, and is independent of bath gas density. In the intermediate and high temperature ranges, we observe a formation signal for ketene (ethenone). The reaction was further investigated by combining the experimental results with quantum chemical calculations and master equation modeling. By making small adjustments (2 − 3 kJ mol −1) to the energies of two key transition states, the model reproduces the experimental results within uncertainties. The experimentally constrained master equation model was used to simulate the CH 3 CCCH • 2 + O 2 reaction system at temperatures and pressures relevant to combustion.
downloadDownload free PDFView PDFchevron_rightChemical Kinetic Studies Using Ultraviolet Cavity Ring-Down Spectroscopic Detection: Self-Reaction of Ethyl and Ethylperoxy Radicals and the Reaction O 2 + C 2 H 5 → C 2 H 5 O 2Dean AtkinsonJ Phys Chem a, 1997
A laser photolysis reactor that uses cavity ring-down spectroscopic (CRDS) detection was characterized and used to measure the rate coefficients of three benchmark reactions of known importance to ethane oxidation. At 295 K and approximately 700 Pa (5.5 Torr) total pressure, we obtained the self-reaction rate coefficients of k ) (1.99 ( 0.44) × 10 -11 cm 3 molecule -1 s -1 for C 2 H 5 + C 2 H 5 and k ) (7.26 ( 2.4) × 10 -14 cm 3 molecule -1 s -1 for C 2 H 5 O 2 + C 2 H 5 O 2 . We obtained k ) (2.7 ( 0.3) × 10 -12 cm 3 molecule -1 s -1 for the pseudo-first-order association reaction O 2 + C 2 H 5 + Ar. We also measured the absorption cross sections of the ethyl radical, σ 220 ) (252 ( 42) × 10 -20 cm 2 molecule -1 and σ 222 ) (206 ( 42) × 10 -20 cm 2 molecule -1 . Stated uncertainties are 2σ. The new rate coefficients agree with those obtained previously by other methods. The agreement confirms that ultraviolet CRDS detection is a viable tool for experimental determinations of gas-phase radical-radical and radical-molecule reaction rate coefficients.
downloadDownload free PDFView PDFchevron_rightThe UV absorption spectrum of the ethylperoxy radical and its self-reaction kinetics between 218 and 333 KGeert MoortgatJournal of Photochemistry and Photobiology A: Chemistry, 1992
The W absorption spectrum of the GH,02 radical between 215 and 295 nm, and the kinetics of its self-reaction in the temperature range 218-333 K were measured using the molecular modulation technique in conjunction with both single wavelength and diode array W spectroscopy.
downloadDownload free PDFView PDFchevron_rightAn experimental and master-equation modeling study of the kinetics of the reaction between resonance-stabilized (CH<sub>3</sub>)<sub>2</sub>CCHCH<sub>2</sub> radical and molecular oxygenRaimo TimonenPhysical Chemistry Chemical Physics, 2021
The kinetics of the reaction between resonance-stabilized (CH 3) 2 CCHCH 2 radical (R) and O 2 has been investigated using photoionization mass spectrometry, and master equation (ME) simulations were performed to support the experimental results. The kinetic measurements of the (CH 3) 2 CCHCH 2 + O 2 reaction (1) were carried out at low helium bath-gas pressures (0.2-5.7 Torr) and over a wide temperature range (238-660 K). Under low temperature (238-298 K) conditions, the pressure-dependent bimolecular association reaction R + O 2-ROO determines kinetics, until at an intermediate temperature range (325-373 K) the ROO adduct becomes thermally unstable and increasingly dissociates back to the reactants with increasing temperature. The initial association of O 2 with (CH 3) 2 CCHCH 2 radical occurs on two distinct sites: terminal 1(t) and non-terminal 1(nt) sites on R, leading to the barrierless formation of ROO (t) and ROO (nt) adducts, respectively. Important for autoignition modelling of olefinic compounds, bimolecular reaction channels appear to open for the R + O 2 reaction at high temperatures (T 4 500 K) and pressureindependent bimolecular rate coefficients of reaction (1) with a weak positive temperature dependence, (2.8-4.6) Â 10 À15 cm 3 molecule À1 s À1 , were measured in the temperature range of 500-660 K. At a temperature of 501 K, a product signal of reaction (1) was observed at m/z = 68, probably originating from isoprene. To explore the reaction mechanism of reaction (1), quantum chemical calculations and ME simulations were performed. According to the ME simulations, without any adjustment to energies, the most important and second most important product channels at the high temperatures are isoprene + HO 2 (yield 4 91%) and (2R/S)-3-methyl-1,2-epoxybut-3-ene + OH (yield o 8%). After modest adjustments to ROO (t) and ROO (nt) well-depths (B0.7 kcal mol À1 each) and barrier height for the transition state associated with the kinetically most dominant channel, R + O 2isoprene + HO 2 (B2.2 kcal mol À1), the ME model was able to reproduce the experimental findings. Modified Arrhenius expressions for the kinetically important reaction channels are enclosed to facilitate the use of current results in combustion models.
downloadDownload free PDFView PDFchevron_rightKinetics of 1-butyl and 2-butyl radical reactions with molecular oxygen: Experiment and theoryRaimo TimonenProceedings of the Combustion Institute, 2019
The reaction of O2 with butyl radicals is a key early step in the oxidation of butane, which is a prototypical alkane fuel with combustion properties that mimic those of many larger alkanes. Current combustion mechanisms employ kinetic descriptions for such radical oxidations that are based on fairly limited information. The present work employs a combination of experiment and theory to probe the kinetics of O2 reacting with both 1and 2-butyl radicals. The experiments employ laser photolysis to generate butyl radicals and thereby initiate the reaction kinetics. Photoionization mass spectrometric observations of the time-dependent butyl radical concentration yield rate constants for the overall reaction. The experiments cover temperatures ranging from 200 to 500 K and He bath gas pressures ranging from to 0.3 to 6 Torr. Ab initio transition state theory (TST) based master equation calculations are used to predict the kinetics over a broad range of conditions. The calculations consider both the barrierless R + O2 entrance channel, treated with direct CASPT2 variable reaction coordinate TST, and the decomposition of the RO2 complex to HO2 + alkenes, treated with CCSD(T)/CBS based TST. Theory and experiment are in good agreement, with maximum discrepancies of about 30 %, suggesting the appropriateness of the theory based predictions for conditions of greater relevance to combustion. The kinetic description arising from this work should be of considerable utility to combustion modeling of butane, as well as of other related saturated hydrocarbons.
downloadDownload free PDFView PDFchevron_rightKinetic data for the reaction of hydroxyl radicals with 1,1,1-trichloroacetaldehyde at 298 ± 2 KOle John NielsenChemical Physics Letters, 1994
The rate constant for the reaction of the hydroxyl radical with l,l, 1-trichloroacetaldehyde has been determined at 298 f. 2 K. Rate data were obtained at atmospheric pressure by a relative rate method. The rate constant was also measured at lower pressures (l-3.4 Torr) using the discharge flow technique with OH radical detection both by resonance fluorescence and electron paramagnetic resonance. The results provide a value of k(OH+CCI,CHO)= (1.1*0.2)x IO-'* cm3 molecule-' s-' at room temperature giving an atmospheric lifetime for CC13CH0 with respect to reaction with OH radicals of 290 h.
downloadDownload free PDFView PDFchevron_rightAn experimental and theoretical study of the kinetics of the reaction between 3-hydroxy-3-methyl-2-butanone and OH radicalsAlexandre TomasRSC Adv., 2015
Absolute experimental and theoretical rate constants are determined for the first time for the reaction of 3hydroxy-3-methyl-2-butanone (3H3M2B) with OH radicals as a function of temperature. Experimental studies were carried out over the temperature range of 277 to 353 K and the pressure range of 5 to 80 Torr, by using a cryogenically cooled cell coupled to the PLP-LIF technique. OH radicals were generated for the first time from the photodissociation of the reactant 3H3M2B at 266 nm and the OH formation yield in 3H3M2B photolysis at 266 nm was measured under our experimental conditions. In addition, the reaction of 3H3M2B with OH radicals was studied theoretically by using the Density Functional Theory (DFT) method under three hydrogen abstraction pathways. According to these calculations, H-atom abstraction occurs more favourably from the methyl group adjacent to the hydroxyl group with a small barrier height. The calculated theoretical rate constants are in good agreement with the experimental data over the temperature range of 278 to 1000 K. No significant temperature dependence can be observed although a very slight effect was observed within the error bars.
downloadDownload free PDFView PDFchevron_rightHydroxyl radical rate constants and photolysis rates of .alpha.-dicarbonylsChristopher PlumEnvironmental Science & Technology, 1983
Photolysis rates of glyoxal, methylglyoxal, and biacetyl and OH radical reaction rate constants for glyoxal and methylglyoxal have been determined at 298 f 2 K in an environmental chamber, by using the photolysis of CH30NO-air mixtures to generate OH radicals. The OH radical rate constants obtained were (1.15 f 0.04) X lo-'' and (1.73 f 0.13) X lo-'' cm3 molecule-l s-' for glyoxal and methylglyoxal, respectively. The photolysis rates of glyoxal, methylglyoxal, and biacetyl increased throughout this series, and average quantum yields for the wavelength region 1290 nm of 0.029 f 0.018,0.107 f 0.030, and 0.158 f 0.024 were derived for glyoxal, methylglyoxal, and biacetyl, respectively. In addition, upper limits to the rate constants for the reaction of O3 with glyoxal and methylglyoxal of <3 X and <6 X cm3 molecule-' s-l, respectively, were obtained at 298 f 2 K. These data will serve as needed input to chemical kinetic computer modeling studies of the aromatic hydrocarbons. Additionally, the a-dicarbonyls also photolyze: of the dicarbonyls and cyclohexane with-0(8P) atoms and o3 were negligible, and since dilution due to sampling was
downloadDownload free PDFView PDFchevron_rightThe kinetics and thermodynamics of free radical reactionsMichael PillingPure and Applied Chemistry, 1992
Three experimental studies are described which emphasise the inter-relastionship of kinetics and thermodynamics. The first involves AH7(t-C4HJ, where descrepancies in experimental values have led to extensive kinetic studies of the reactions t-C4€& + HX (X = Br, I) which surprisingly have negative activation energies. The second study relates to forward and reverse reactions in the system H + HBr + H2 + Br where use of the equilibrium constant enables rate parameters for both reactions to be defined over a very wide temperature range. Finally, recent direct measurements are reported on the rate constant for the neopentyl peroxy + hydroperoxy radical isomerisation. The results demonstrate an overestimate of the rate constant in previous indirect studies, which can be ascribed to the use of inaccurate thermodynamic data.
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downloadDownload free PDFView PDFchevron_rightTemperature Dependence Study of the Kinetics and Product Yields of the HO2 + CH3C(O)O2 Reaction by Direct Detection of OH and HO2 Radicals Using 2f-IR Wavelength Modulation SpectroscopyMitchio OkumuraThe Journal of Physical Chemistry A
downloadDownload free PDFView PDFchevron_rightKinetics of the Reactions of CH<sub>2</sub>Cl, CH<sub>3</sub>CHCl, and CH<sub>3</sub>CCl<sub>2</sub> Radicals with Cl<sub>2</sub> in the Temperature Range 191−363 KRaimo TimonenJournal of Physical Chemistry A, 2010
The kinetics of three chlorinated free radical reactions with Cl 2 have been studied in direct time-resolved measurements. Radicals were produced in low initial concentrations by pulsed laser photolysis at 193 nm, and the subsequent decays of the radical concentrations were measured under pseudo-first-order conditions using photoionization mass spectrometer (PIMS). The bimolecular rate coefficients of the CH 3 CHCl + Cl 2 reaction obtained from the current measurements exhibit negative temperature dependence and can be expressed by the equation k(CH 3 CHCl + Cl 2)) ((3.02 (0.14) × 10-12)(T/300 K)-1.89(0.19 cm 3 molecule-1 s-1 (1.7-5.4 Torr, 191-363 K). For the CH 3 CCl 2 + Cl 2 reaction the current results could be fitted with the equation k(CH 3 CCl 2 + Cl 2)) ((1.23 (0.02) × 10-13)(T/300 K)-0.26(0.10 cm 3 molecule-1 s-1 (3.9-5.1 Torr, 240-363 K). The measured rate coefficients for the CH 2 Cl + Cl 2 reaction plotted as a function of temperature show a minimum at about T) 240 K: first decreasing with increasing temperature and then, above the limit, increasing with temperature. The determined reaction rate coefficients can be expressed as k(CH 2 Cl + Cl 2)) ((2.11 (1.29) × 10-14) exp(773 (183 K/T)(T/300 K) 3.26(0.67 cm 3 molecule-1 s-1 (4.0-5.6 Torr, 201-363 K). The rate coefficients for the CH 3 CCl 2 + Cl 2 and CH 2 Cl + Cl 2 reactions can be combined with previous results to obtain: k combined (CH 3 CCl 2 + Cl 2)) ((4.72 (1.66) × 10-15) exp(971 (106 K/T)(T/300 K) 3.07(0.23 cm 3 molecule-1 s-1 (3.1-7.4 Torr, 240-873 K) and k combined (CH 2 Cl + Cl 2)) ((5.18 (1.06) × 10-14) exp(525 (63 K/T)(T/300 K) 2.52(0.13 cm 3 molecule-1 s-1 (1.8-5.6 Torr, 201-873 K). All the uncertainties given refer only to the 1σ statistical uncertainties obtained from the fitting, and the estimated overall uncertainty in the determined bimolecular rate coefficients is about (15%.
downloadDownload free PDFView PDFchevron_rightOxidation of dimethyl ether: Absolute rate constants for the self reaction of CH3OCH2 radicals, the reaction of CH3OCH2 radicals with O2, and the thermal decomposition of CH3OCH2 radicalsOle John NielsenInternational Journal of Chemical Kinetics, 1997
The rate constant for the reaction of CH 3 OCH 2 radicals with O 2 (reaction (1)) and the self reaction of CH 3 OCH 2 radicals (reaction (5)) were measured using pulse radiolysis coupled with time resolved UV absorption spectroscopy. k 1 was studied at 296 K over the pressure range 0.025-1 bar and in the temperature range 296-473 K at 18 bar total pressure. Reaction (1) is known to proceed through the following mechanism: (k prod) (k RO2) where k RO2 is the rate constant for peroxy radical production and k prod is the rate constant for formaldehyde production. The k 1 values obtained at 296 K together with the available literature values for k 1 determined at low pressures were fitted using a modified Lindemann mechanism and the following parameters were obtained: cm 6 cm 3 and cm 3 where k RO2,0 and k RO2,ϱ are the overall termolecular and bimolecular rate constants for formation of CH 3 OCH 2 O 2 rad-s Ϫ1 molecule Ϫ1 k prod,0 ϭ (6.0 Ϯ 0.5) ϫ 10 Ϫ12 s Ϫ1 , molecule Ϫ1 k RO2,ϱ ϭ (1.14 Ϯ 0.04) ϫ 10 Ϫ11 s Ϫ1 , molecule Ϫ2 k RO2,0 ϭ (9.4 Ϯ 4.2) ϫ 10 Ϫ30 k 1 ϭ k RO2 ϩ k prod , CH 3 OCH 2 O 2 # ϩ M 9: CH 3 OCH 2 O 2 ϩ M CH 3 OCH 2 ϩ O 2 ;: CH 3 OCH 2 O 2 # 9: CH 2 OCH 2 O 2 H # 9: 2HCHO ϩ OH CH 3 OCH 2 ϩ O 2 ;: 628 SEHESTED ET AL. icals and k prod,0 represents the bimolecular rate constant for the reaction of CH 3 OCH 2 radicals with O 2 to yield formaldehyde in the limit of low pressure. exp cm 3 was determined at 18 bar total pressure over the temperature range 296-473 K. At 1 bar total pressure and 296 K, cm 3 and at 18 bar total pressure over the temperature range 296-523 K, cm 3 As a part of this study the decay rate of CH 3 OCH 2 radicals was used to study the thermal decomposition of CH 3 OCH 2 radicals in the temperature range 573-666 K at 18 bar total pressure. The observed decay rates of CH 3 OCH 2 radicals were consistent with the literature value of The results are discussed in the context of dimethyl ether as an alternative diesel fuel.
downloadDownload free PDFView PDFchevron_rightA Kinetic Study On The Reactions Of OH Radicals With Esters And Alkoxy EstersStéphane Le CalvéWIT Transactions on Ecology and the Environment, 1970
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