{"title":"氢氧加成C2H2和C2H4的高压范围","authors":"D. Fulle, H.F. Hamann, H. Hippler, C.P. Jänsch","doi":"10.1002/bbpc.199700004","DOIUrl":null,"url":null,"abstract":"<p>The kinetics of the bimolecular reactions OH+C<sub>2</sub>H<sub>2</sub>+M ⟺ C<sub>2</sub>H<sub>2</sub>OH+M (1) and OH+C<sub>2</sub>H<sub>4</sub>+M ⟺ C<sub>2</sub>H<sub>4</sub>OH+M (2) have been investigated over an extended pressure (1–130 bar) and temperature (300–800 K) range. The OH radicals have been generated by laser flash photolysis of suited precursors and their decays have been measured by saturated laser-induced fluorescence (SLIF) under pseudo-first-order conditions. The pressure dependences have been analyzed by constructing falloff curves at fixed temperatures leading to reliable extrapolations towards the high pressure limiting rate constants <i>k</i><sub>∞</sub>. In the given temperature range these rate constants are represented as <i>k</i><sub>1,∞</sub> = 3.8×10<sup>−11</sup> exp (–910 K/<i>T</i>) cm<sup>3</sup> molecule<sup>−1</sup> s<sup>−1</sup> and as <i>k</i><sub>2,∞</sub> = 1.0×10<sup>−11</sup> cm<sup>3</sup> molecule<sup>−1</sup> s<sup>−1</sup>. At temperatures above 700 K biexponential decay curves have been obtained. The chemical equilibria of reactions (1) and (2) could be determined. By a third law analysis the equilibrium constants have been evaluated with reaction enthalpies for the addition complex C<sub>2</sub>H<sub>2</sub>OH of δ<sub>I</sub>H<sup>o</sup><sub>1</sub> (O K) = -(146 ± 10) kJ/mol and for C<sub>2</sub>H<sub>4</sub>OH of δ<sub>I</sub>H<sup>o</sup><sub>2</sub> (O K) = -(123 ± 6) kJ/mol, respectively. The two equilibrium constants are given by <i>K</i><sub>1,eq</sub> = (5.4±2.2)×10<sup>−2</sup> (<i>T</i>/K)<sup>−1.7±0.2</sup> exp ((17560±1200) K/<i>T</i>) bar<sup>−1</sup> and <i>K</i><sub>2,eq</sub> = 2.1 × 10<sup>−2</sup> (T/K)<sup>−95±0.1</sup> × exp ((14780±720) K/<i>T</i>) bar<sup>−1</sup>, respectively.</p>","PeriodicalId":100156,"journal":{"name":"Berichte der Bunsengesellschaft für physikalische Chemie","volume":"101 10","pages":"1433-1442"},"PeriodicalIF":0.0000,"publicationDate":"2014-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1002/bbpc.199700004","citationCount":"29","resultStr":"{\"title\":\"The High Pressure Range of the Addition of OH to C2H2 and C2H4\",\"authors\":\"D. Fulle, H.F. Hamann, H. Hippler, C.P. Jänsch\",\"doi\":\"10.1002/bbpc.199700004\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The kinetics of the bimolecular reactions OH+C<sub>2</sub>H<sub>2</sub>+M ⟺ C<sub>2</sub>H<sub>2</sub>OH+M (1) and OH+C<sub>2</sub>H<sub>4</sub>+M ⟺ C<sub>2</sub>H<sub>4</sub>OH+M (2) have been investigated over an extended pressure (1–130 bar) and temperature (300–800 K) range. The OH radicals have been generated by laser flash photolysis of suited precursors and their decays have been measured by saturated laser-induced fluorescence (SLIF) under pseudo-first-order conditions. The pressure dependences have been analyzed by constructing falloff curves at fixed temperatures leading to reliable extrapolations towards the high pressure limiting rate constants <i>k</i><sub>∞</sub>. In the given temperature range these rate constants are represented as <i>k</i><sub>1,∞</sub> = 3.8×10<sup>−11</sup> exp (–910 K/<i>T</i>) cm<sup>3</sup> molecule<sup>−1</sup> s<sup>−1</sup> and as <i>k</i><sub>2,∞</sub> = 1.0×10<sup>−11</sup> cm<sup>3</sup> molecule<sup>−1</sup> s<sup>−1</sup>. At temperatures above 700 K biexponential decay curves have been obtained. The chemical equilibria of reactions (1) and (2) could be determined. By a third law analysis the equilibrium constants have been evaluated with reaction enthalpies for the addition complex C<sub>2</sub>H<sub>2</sub>OH of δ<sub>I</sub>H<sup>o</sup><sub>1</sub> (O K) = -(146 ± 10) kJ/mol and for C<sub>2</sub>H<sub>4</sub>OH of δ<sub>I</sub>H<sup>o</sup><sub>2</sub> (O K) = -(123 ± 6) kJ/mol, respectively. The two equilibrium constants are given by <i>K</i><sub>1,eq</sub> = (5.4±2.2)×10<sup>−2</sup> (<i>T</i>/K)<sup>−1.7±0.2</sup> exp ((17560±1200) K/<i>T</i>) bar<sup>−1</sup> and <i>K</i><sub>2,eq</sub> = 2.1 × 10<sup>−2</sup> (T/K)<sup>−95±0.1</sup> × exp ((14780±720) K/<i>T</i>) bar<sup>−1</sup>, respectively.</p>\",\"PeriodicalId\":100156,\"journal\":{\"name\":\"Berichte der Bunsengesellschaft für physikalische Chemie\",\"volume\":\"101 10\",\"pages\":\"1433-1442\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2014-03-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1002/bbpc.199700004\",\"citationCount\":\"29\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Berichte der Bunsengesellschaft für physikalische Chemie\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/bbpc.199700004\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Berichte der Bunsengesellschaft für physikalische Chemie","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/bbpc.199700004","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The High Pressure Range of the Addition of OH to C2H2 and C2H4
The kinetics of the bimolecular reactions OH+C2H2+M ⟺ C2H2OH+M (1) and OH+C2H4+M ⟺ C2H4OH+M (2) have been investigated over an extended pressure (1–130 bar) and temperature (300–800 K) range. The OH radicals have been generated by laser flash photolysis of suited precursors and their decays have been measured by saturated laser-induced fluorescence (SLIF) under pseudo-first-order conditions. The pressure dependences have been analyzed by constructing falloff curves at fixed temperatures leading to reliable extrapolations towards the high pressure limiting rate constants k∞. In the given temperature range these rate constants are represented as k1,∞ = 3.8×10−11 exp (–910 K/T) cm3 molecule−1 s−1 and as k2,∞ = 1.0×10−11 cm3 molecule−1 s−1. At temperatures above 700 K biexponential decay curves have been obtained. The chemical equilibria of reactions (1) and (2) could be determined. By a third law analysis the equilibrium constants have been evaluated with reaction enthalpies for the addition complex C2H2OH of δIHo1 (O K) = -(146 ± 10) kJ/mol and for C2H4OH of δIHo2 (O K) = -(123 ± 6) kJ/mol, respectively. The two equilibrium constants are given by K1,eq = (5.4±2.2)×10−2 (T/K)−1.7±0.2 exp ((17560±1200) K/T) bar−1 and K2,eq = 2.1 × 10−2 (T/K)−95±0.1 × exp ((14780±720) K/T) bar−1, respectively.