Disproportionation Channel of the Self-reaction of Hydroxyl Radical, OH + OH → H2O + O, Revisited
The rate constant of the disproportionation channel 1a of the self-reaction of hydroxyl radicals OH + OH → H2O + O (1a) was measured at ambient temperature as well as over an extended temperature range to resolve the discrepancy between the IUPAC recommended value (k 1a = 1.48 × 10–12 cm3 molecule–1...
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Veröffentlicht in: | The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2020-05, Vol.124 (20), p.3993-4005 |
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description | The rate constant of the disproportionation channel 1a of the self-reaction of hydroxyl radicals OH + OH → H2O + O (1a) was measured at ambient temperature as well as over an extended temperature range to resolve the discrepancy between the IUPAC recommended value (k 1a = 1.48 × 10–12 cm3 molecule–1 s–1, discharge flow system, Bedjanian et al. J. Phys. Chem. A 1999, 103, 7017 ) and a factor of ca. 1.8 higher value by pulsed laser photolysis (2.7 × 10–12 cm3 molecule–1 s–1, Bahng et al. J. Phys. Chem. A 2007, 111, 3850 , and 2.52 × 10–12 cm3 molecule–1 s–1, Altinay et al. J. Phys. Chem. A 2014, 118, 38 ). To resolve this discrepancy, the rate constant of the title reaction was remeasured in three laboratories using two different experimental techniques, namely, laser-pulsed photolysis–transient UV absorption and fast discharge flow system coupled with mass spectrometry. Two different precursors were used to generate OH radicals in the laser-pulsed photolysis experiments. The experiments confirmed the low value of the rate constant at ambient temperature (k 1a = (1.4 ± 0.2) × 10–12 cm3 molecule–1 s–1 at 295 K) as well as the V-shaped temperature dependence, negative at low temperatures and positive at high temperatures, with a turning point at 427 K: k 1a = 8.38 × 10–14 × (T/300)1.99 × exp(855/T) cm3 molecule–1 s–1 (220–950 K). Recommended expression over the 220–2384 K temperature range: k 1a = 2.68 × 10–14 × (T/300)2.75 × exp(1165/T) cm3 molecule–1 s–1 (220–2384 K). |
doi_str_mv | 10.1021/acs.jpca.0c00624 |
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J. Phys. Chem. A 1999, 103, 7017 ) and a factor of ca. 1.8 higher value by pulsed laser photolysis (2.7 × 10–12 cm3 molecule–1 s–1, Bahng et al. J. Phys. Chem. A 2007, 111, 3850 , and 2.52 × 10–12 cm3 molecule–1 s–1, Altinay et al. J. Phys. Chem. A 2014, 118, 38 ). To resolve this discrepancy, the rate constant of the title reaction was remeasured in three laboratories using two different experimental techniques, namely, laser-pulsed photolysis–transient UV absorption and fast discharge flow system coupled with mass spectrometry. Two different precursors were used to generate OH radicals in the laser-pulsed photolysis experiments. The experiments confirmed the low value of the rate constant at ambient temperature (k 1a = (1.4 ± 0.2) × 10–12 cm3 molecule–1 s–1 at 295 K) as well as the V-shaped temperature dependence, negative at low temperatures and positive at high temperatures, with a turning point at 427 K: k 1a = 8.38 × 10–14 × (T/300)1.99 × exp(855/T) cm3 molecule–1 s–1 (220–950 K). Recommended expression over the 220–2384 K temperature range: k 1a = 2.68 × 10–14 × (T/300)2.75 × exp(1165/T) cm3 molecule–1 s–1 (220–2384 K).</description><identifier>ISSN: 1089-5639</identifier><identifier>EISSN: 1520-5215</identifier><identifier>DOI: 10.1021/acs.jpca.0c00624</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>The journal of physical chemistry. 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A, Molecules, spectroscopy, kinetics, environment, & general theory</title><addtitle>J. Phys. Chem. A</addtitle><description>The rate constant of the disproportionation channel 1a of the self-reaction of hydroxyl radicals OH + OH → H2O + O (1a) was measured at ambient temperature as well as over an extended temperature range to resolve the discrepancy between the IUPAC recommended value (k 1a = 1.48 × 10–12 cm3 molecule–1 s–1, discharge flow system, Bedjanian et al. J. Phys. Chem. A 1999, 103, 7017 ) and a factor of ca. 1.8 higher value by pulsed laser photolysis (2.7 × 10–12 cm3 molecule–1 s–1, Bahng et al. J. Phys. Chem. A 2007, 111, 3850 , and 2.52 × 10–12 cm3 molecule–1 s–1, Altinay et al. J. Phys. Chem. A 2014, 118, 38 ). To resolve this discrepancy, the rate constant of the title reaction was remeasured in three laboratories using two different experimental techniques, namely, laser-pulsed photolysis–transient UV absorption and fast discharge flow system coupled with mass spectrometry. Two different precursors were used to generate OH radicals in the laser-pulsed photolysis experiments. The experiments confirmed the low value of the rate constant at ambient temperature (k 1a = (1.4 ± 0.2) × 10–12 cm3 molecule–1 s–1 at 295 K) as well as the V-shaped temperature dependence, negative at low temperatures and positive at high temperatures, with a turning point at 427 K: k 1a = 8.38 × 10–14 × (T/300)1.99 × exp(855/T) cm3 molecule–1 s–1 (220–950 K). Recommended expression over the 220–2384 K temperature range: k 1a = 2.68 × 10–14 × (T/300)2.75 × exp(1165/T) cm3 molecule–1 s–1 (220–2384 K).</description><issn>1089-5639</issn><issn>1520-5215</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNotUMtOwzAQtBBIlMKdo49INGX9SpojKo8gVapU4Gw5tqOmMnGJE0R_gA_gE_kSnLaX2d3Z1e7sIHRNYEqAkjulw3Sz1WoKGiCl_ASNiKCQCErEacxhliciZfk5ughhAwCEUT5C-qEO29ZvfdvVvlED4PlaNY112Fe4W1v8al2VtFbpfTOSxc60_nvn8EqZWis3wcsC3w7w9_OLC7ocigle2a861J01l-isUi7Yq2Mco_enx7d5kSyWzy_z-0WiyIzyxELGTGlApdpUZUk1mNRYSqwAlhmaGRMlm5JQYHzGic1KkzNSCUFpnhPN2BjdHPbGhz57Gzr5UQdtnVON9X2QlEM8JHLC4-jkMBptkxvft00UJgnIwUu5J6OX8ugl-wfJz2el</recordid><startdate>20200521</startdate><enddate>20200521</enddate><creator>Zhang, Xiaokai</creator><creator>Sangwan, Manuvesh</creator><creator>Yan, Chao</creator><creator>Koshlyakov, Pavel V</creator><creator>Chesnokov, Evgeni N</creator><creator>Bedjanian, Yuri</creator><creator>Krasnoperov, Lev N</creator><general>American Chemical Society</general><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-5383-5130</orcidid><orcidid>https://orcid.org/0000-0002-3693-6092</orcidid><orcidid>https://orcid.org/0000-0002-2415-6080</orcidid></search><sort><creationdate>20200521</creationdate><title>Disproportionation Channel of the Self-reaction of Hydroxyl Radical, OH + OH → H2O + O, Revisited</title><author>Zhang, Xiaokai ; Sangwan, Manuvesh ; Yan, Chao ; Koshlyakov, Pavel V ; Chesnokov, Evgeni N ; Bedjanian, Yuri ; Krasnoperov, Lev N</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a1824-e073dbd0a6cdfbb2c0d6de21e5037d27dd132db12034841e7bd931f5522991c33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhang, Xiaokai</creatorcontrib><creatorcontrib>Sangwan, Manuvesh</creatorcontrib><creatorcontrib>Yan, Chao</creatorcontrib><creatorcontrib>Koshlyakov, Pavel V</creatorcontrib><creatorcontrib>Chesnokov, Evgeni N</creatorcontrib><creatorcontrib>Bedjanian, Yuri</creatorcontrib><creatorcontrib>Krasnoperov, Lev N</creatorcontrib><collection>MEDLINE - Academic</collection><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhang, Xiaokai</au><au>Sangwan, Manuvesh</au><au>Yan, Chao</au><au>Koshlyakov, Pavel V</au><au>Chesnokov, Evgeni N</au><au>Bedjanian, Yuri</au><au>Krasnoperov, Lev N</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Disproportionation Channel of the Self-reaction of Hydroxyl Radical, OH + OH → H2O + O, Revisited</atitle><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory</jtitle><addtitle>J. Phys. Chem. A</addtitle><date>2020-05-21</date><risdate>2020</risdate><volume>124</volume><issue>20</issue><spage>3993</spage><epage>4005</epage><pages>3993-4005</pages><issn>1089-5639</issn><eissn>1520-5215</eissn><abstract>The rate constant of the disproportionation channel 1a of the self-reaction of hydroxyl radicals OH + OH → H2O + O (1a) was measured at ambient temperature as well as over an extended temperature range to resolve the discrepancy between the IUPAC recommended value (k 1a = 1.48 × 10–12 cm3 molecule–1 s–1, discharge flow system, Bedjanian et al. J. Phys. Chem. A 1999, 103, 7017 ) and a factor of ca. 1.8 higher value by pulsed laser photolysis (2.7 × 10–12 cm3 molecule–1 s–1, Bahng et al. J. Phys. Chem. A 2007, 111, 3850 , and 2.52 × 10–12 cm3 molecule–1 s–1, Altinay et al. J. Phys. Chem. A 2014, 118, 38 ). To resolve this discrepancy, the rate constant of the title reaction was remeasured in three laboratories using two different experimental techniques, namely, laser-pulsed photolysis–transient UV absorption and fast discharge flow system coupled with mass spectrometry. Two different precursors were used to generate OH radicals in the laser-pulsed photolysis experiments. The experiments confirmed the low value of the rate constant at ambient temperature (k 1a = (1.4 ± 0.2) × 10–12 cm3 molecule–1 s–1 at 295 K) as well as the V-shaped temperature dependence, negative at low temperatures and positive at high temperatures, with a turning point at 427 K: k 1a = 8.38 × 10–14 × (T/300)1.99 × exp(855/T) cm3 molecule–1 s–1 (220–950 K). Recommended expression over the 220–2384 K temperature range: k 1a = 2.68 × 10–14 × (T/300)2.75 × exp(1165/T) cm3 molecule–1 s–1 (220–2384 K).</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.jpca.0c00624</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0001-5383-5130</orcidid><orcidid>https://orcid.org/0000-0002-3693-6092</orcidid><orcidid>https://orcid.org/0000-0002-2415-6080</orcidid><oa>free_for_read</oa></addata></record> |
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title | Disproportionation Channel of the Self-reaction of Hydroxyl Radical, OH + OH → H2O + O, Revisited |
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