Mohammad Adil , Binod Raj Giri , Tam V.-T. Mai , Milán Szőri , Lam K. Huynh , Aamir Farooq
{"title":"2-甲基-1,3-二恶氧烷的高温中红外吸收及反应动力学的实验与理论研究","authors":"Mohammad Adil , Binod Raj Giri , Tam V.-T. Mai , Milán Szőri , Lam K. Huynh , Aamir Farooq","doi":"10.1016/j.jpap.2023.100165","DOIUrl":null,"url":null,"abstract":"<div><p>This work reports the mid-IR spectroscopy and reaction kinetics of 2-methyl-1,3-dioxolane (2M13DO). We carried out spectroscopic measurements to deduce temperature-dependent absorption cross-sections of 2M13DO over a broad wavelength range of 8.4–10.5 μm (950–1190 cm<sup>−1</sup>). For these measurements, we employed a rapidly tuning MIRcat-QT™ laser that can be operated either at a fixed wavelength or scanned mode over wide wavelength regions. By operating the laser at a fixed wavelength, we monitored the decay of 2M13DO behind reflected shock waves over <em>T</em><sub>5</sub> = 1050–1400 K and <em>P</em><sub>5</sub> = 0.7 and 2.6 bar. Our measured concentration time-histories of 2M13DO allowed us to directly extract the overall rate coefficients for the unimolecular decomposition of 2M13DO using the first-order rate law. We did not observe any pressure dependence in the measured rate coefficients, indicating that the reaction is close to the high-pressure limit. By employing the W1U composite method, we explored the important pyrolysis reaction pathways of 2M13DO in the reactive potential energy surface. Three important reaction channels, namely, 2M13DO → CH<sub>2</sub><img>CHOCH<sub>2</sub>CH<sub>2</sub>OH (<strong>IM1</strong>), 2M13DO → 2CH<sub>3</sub>CHO (<strong>P3</strong>), 2M13DO → CH<sub>3</sub> + 1,3-dioxolan-2-yl (<strong>P4</strong>) were identified. Below 700 K, <strong>IM1</strong> forming channel is dominant, whereas CH<sub>3</sub>CHO formation is dominant under our experimental conditions. Above 1500 K, the radical forming channel (CH<sub>3</sub>+<strong>P4</strong>) takes over other channels. At higher temperatures, the contribution of the radical forming channel continually increases, accounting for ∼ 99% at 2000 K. We used the stochastic RRKM-ME model to predict the pressure and temperature dependence of the rate coefficients, <em>k</em>(<em>T, P</em>), and time-resolved species profiles. Our theory showed excellent agreement with the measured rate coefficients. These are the first direct determination of the rate coefficients of the unimolecular decomposition of 2M13DO.</p></div>","PeriodicalId":375,"journal":{"name":"Journal of Photochemistry and Photobiology","volume":"13 ","pages":"Article 100165"},"PeriodicalIF":3.2610,"publicationDate":"2023-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"High-temperature mid-IR absorption and reaction kinetics of 2-methyl-1,3-dioxolane: An experimental and theoretical study\",\"authors\":\"Mohammad Adil , Binod Raj Giri , Tam V.-T. Mai , Milán Szőri , Lam K. Huynh , Aamir Farooq\",\"doi\":\"10.1016/j.jpap.2023.100165\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>This work reports the mid-IR spectroscopy and reaction kinetics of 2-methyl-1,3-dioxolane (2M13DO). We carried out spectroscopic measurements to deduce temperature-dependent absorption cross-sections of 2M13DO over a broad wavelength range of 8.4–10.5 μm (950–1190 cm<sup>−1</sup>). For these measurements, we employed a rapidly tuning MIRcat-QT™ laser that can be operated either at a fixed wavelength or scanned mode over wide wavelength regions. By operating the laser at a fixed wavelength, we monitored the decay of 2M13DO behind reflected shock waves over <em>T</em><sub>5</sub> = 1050–1400 K and <em>P</em><sub>5</sub> = 0.7 and 2.6 bar. Our measured concentration time-histories of 2M13DO allowed us to directly extract the overall rate coefficients for the unimolecular decomposition of 2M13DO using the first-order rate law. We did not observe any pressure dependence in the measured rate coefficients, indicating that the reaction is close to the high-pressure limit. By employing the W1U composite method, we explored the important pyrolysis reaction pathways of 2M13DO in the reactive potential energy surface. Three important reaction channels, namely, 2M13DO → CH<sub>2</sub><img>CHOCH<sub>2</sub>CH<sub>2</sub>OH (<strong>IM1</strong>), 2M13DO → 2CH<sub>3</sub>CHO (<strong>P3</strong>), 2M13DO → CH<sub>3</sub> + 1,3-dioxolan-2-yl (<strong>P4</strong>) were identified. Below 700 K, <strong>IM1</strong> forming channel is dominant, whereas CH<sub>3</sub>CHO formation is dominant under our experimental conditions. Above 1500 K, the radical forming channel (CH<sub>3</sub>+<strong>P4</strong>) takes over other channels. At higher temperatures, the contribution of the radical forming channel continually increases, accounting for ∼ 99% at 2000 K. We used the stochastic RRKM-ME model to predict the pressure and temperature dependence of the rate coefficients, <em>k</em>(<em>T, P</em>), and time-resolved species profiles. Our theory showed excellent agreement with the measured rate coefficients. These are the first direct determination of the rate coefficients of the unimolecular decomposition of 2M13DO.</p></div>\",\"PeriodicalId\":375,\"journal\":{\"name\":\"Journal of Photochemistry and Photobiology\",\"volume\":\"13 \",\"pages\":\"Article 100165\"},\"PeriodicalIF\":3.2610,\"publicationDate\":\"2023-02-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Photochemistry and Photobiology\",\"FirstCategoryId\":\"2\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2666469023000064\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Photochemistry and Photobiology","FirstCategoryId":"2","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2666469023000064","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
High-temperature mid-IR absorption and reaction kinetics of 2-methyl-1,3-dioxolane: An experimental and theoretical study
This work reports the mid-IR spectroscopy and reaction kinetics of 2-methyl-1,3-dioxolane (2M13DO). We carried out spectroscopic measurements to deduce temperature-dependent absorption cross-sections of 2M13DO over a broad wavelength range of 8.4–10.5 μm (950–1190 cm−1). For these measurements, we employed a rapidly tuning MIRcat-QT™ laser that can be operated either at a fixed wavelength or scanned mode over wide wavelength regions. By operating the laser at a fixed wavelength, we monitored the decay of 2M13DO behind reflected shock waves over T5 = 1050–1400 K and P5 = 0.7 and 2.6 bar. Our measured concentration time-histories of 2M13DO allowed us to directly extract the overall rate coefficients for the unimolecular decomposition of 2M13DO using the first-order rate law. We did not observe any pressure dependence in the measured rate coefficients, indicating that the reaction is close to the high-pressure limit. By employing the W1U composite method, we explored the important pyrolysis reaction pathways of 2M13DO in the reactive potential energy surface. Three important reaction channels, namely, 2M13DO → CH2CHOCH2CH2OH (IM1), 2M13DO → 2CH3CHO (P3), 2M13DO → CH3 + 1,3-dioxolan-2-yl (P4) were identified. Below 700 K, IM1 forming channel is dominant, whereas CH3CHO formation is dominant under our experimental conditions. Above 1500 K, the radical forming channel (CH3+P4) takes over other channels. At higher temperatures, the contribution of the radical forming channel continually increases, accounting for ∼ 99% at 2000 K. We used the stochastic RRKM-ME model to predict the pressure and temperature dependence of the rate coefficients, k(T, P), and time-resolved species profiles. Our theory showed excellent agreement with the measured rate coefficients. These are the first direct determination of the rate coefficients of the unimolecular decomposition of 2M13DO.