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Recombination of Allyl Radicals in the High Temperature Fall-Off Regime

The recombination of allyl radicals (C3H5), generated from the dissociation of 1,5-hexadiene or allyl iodide dilute in krypton, has been investigated in a diaphragmless shock tube using laser schlieren densitometry, LS, (900–1700 K, 10 ± 1, 29 ± 3, 57 ± 3, and 120 ± 4 Torr). The LS density gradient...

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Published in:The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2013-06, Vol.117 (23), p.4750-4761
Main Authors: Lynch, Patrick T, Annesley, Christopher J, Aul, Christopher J, Yang, Xueliang, Tranter, Robert S
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container_title The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
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creator Lynch, Patrick T
Annesley, Christopher J
Aul, Christopher J
Yang, Xueliang
Tranter, Robert S
description The recombination of allyl radicals (C3H5), generated from the dissociation of 1,5-hexadiene or allyl iodide dilute in krypton, has been investigated in a diaphragmless shock tube using laser schlieren densitometry, LS, (900–1700 K, 10 ± 1, 29 ± 3, 57 ± 3, and 120 ± 4 Torr). The LS density gradient profiles were simulated and excellent agreement was found between simulations and experimental profiles. Rate coefficients for C3H5I → C3H5 + I and C3H5 + C3H5 → C6H10 were obtained and showed strong fall-off. Second order rate coefficients for allyl radical recombination were determined as k 1a,124Torr = (2.6 ± 0.8) × 1055 T  –12.995 exp(−8426/T), k 1a,57Torr = (1.7 ± 0.5) × 1060 T  –14.49 exp(−9344/T), and k 1a,30Torr = (7.5 ± 2.3) × 1066 T  –15.935 exp(−10192/T) cm3 mol–1s–1. The contribution of a disproportionation channel in allyl radical reactions was assessed, and the best agreement was obtained with no more than 5% disproportionation. Notably, because both the forward and back reactions of C6H10 ⇌ C3H5 + C3H5 were measured, utilizing two different precursors, the equilibrium constant of this reaction could be found, suggesting an entropy of formation of 1,5-hexadiene, 87.3 cal mol–1 K–1, which is significantly smaller than that group additivity predicts, but larger than other reference literature values.
doi_str_mv 10.1021/jp402484v
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The LS density gradient profiles were simulated and excellent agreement was found between simulations and experimental profiles. Rate coefficients for C3H5I → C3H5 + I and C3H5 + C3H5 → C6H10 were obtained and showed strong fall-off. Second order rate coefficients for allyl radical recombination were determined as k 1a,124Torr = (2.6 ± 0.8) × 1055 T  –12.995 exp(−8426/T), k 1a,57Torr = (1.7 ± 0.5) × 1060 T  –14.49 exp(−9344/T), and k 1a,30Torr = (7.5 ± 2.3) × 1066 T  –15.935 exp(−10192/T) cm3 mol–1s–1. The contribution of a disproportionation channel in allyl radical reactions was assessed, and the best agreement was obtained with no more than 5% disproportionation. 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A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</title><addtitle>J. Phys. Chem. A</addtitle><description>The recombination of allyl radicals (C3H5), generated from the dissociation of 1,5-hexadiene or allyl iodide dilute in krypton, has been investigated in a diaphragmless shock tube using laser schlieren densitometry, LS, (900–1700 K, 10 ± 1, 29 ± 3, 57 ± 3, and 120 ± 4 Torr). The LS density gradient profiles were simulated and excellent agreement was found between simulations and experimental profiles. Rate coefficients for C3H5I → C3H5 + I and C3H5 + C3H5 → C6H10 were obtained and showed strong fall-off. Second order rate coefficients for allyl radical recombination were determined as k 1a,124Torr = (2.6 ± 0.8) × 1055 T  –12.995 exp(−8426/T), k 1a,57Torr = (1.7 ± 0.5) × 1060 T  –14.49 exp(−9344/T), and k 1a,30Torr = (7.5 ± 2.3) × 1066 T  –15.935 exp(−10192/T) cm3 mol–1s–1. 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A</addtitle><date>2013-06-13</date><risdate>2013</risdate><volume>117</volume><issue>23</issue><spage>4750</spage><epage>4761</epage><pages>4750-4761</pages><issn>1089-5639</issn><eissn>1520-5215</eissn><abstract>The recombination of allyl radicals (C3H5), generated from the dissociation of 1,5-hexadiene or allyl iodide dilute in krypton, has been investigated in a diaphragmless shock tube using laser schlieren densitometry, LS, (900–1700 K, 10 ± 1, 29 ± 3, 57 ± 3, and 120 ± 4 Torr). The LS density gradient profiles were simulated and excellent agreement was found between simulations and experimental profiles. Rate coefficients for C3H5I → C3H5 + I and C3H5 + C3H5 → C6H10 were obtained and showed strong fall-off. Second order rate coefficients for allyl radical recombination were determined as k 1a,124Torr = (2.6 ± 0.8) × 1055 T  –12.995 exp(−8426/T), k 1a,57Torr = (1.7 ± 0.5) × 1060 T  –14.49 exp(−9344/T), and k 1a,30Torr = (7.5 ± 2.3) × 1066 T  –15.935 exp(−10192/T) cm3 mol–1s–1. The contribution of a disproportionation channel in allyl radical reactions was assessed, and the best agreement was obtained with no more than 5% disproportionation. Notably, because both the forward and back reactions of C6H10 ⇌ C3H5 + C3H5 were measured, utilizing two different precursors, the equilibrium constant of this reaction could be found, suggesting an entropy of formation of 1,5-hexadiene, 87.3 cal mol–1 K–1, which is significantly smaller than that group additivity predicts, but larger than other reference literature values.</abstract><cop>Washington, DC</cop><pub>American Chemical Society</pub><pmid>23679185</pmid><doi>10.1021/jp402484v</doi><tpages>12</tpages></addata></record>
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source American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list)
subjects Allyl Compounds - chemistry
Channels
Chemistry
Densitometry
Disproportionation
Exact sciences and technology
Free Radicals - chemistry
Iodides
Kinetics and mechanisms
Lasers
Molecular Structure
Organic chemistry
Precursors
Radicals
Reactivity and mechanisms
Simulation
Temperature
title Recombination of Allyl Radicals in the High Temperature Fall-Off Regime
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