{"title":"硝酸乙酯气相溶剂化NO2 -和NO3 -","authors":"S. Włodek, Z. Łuczyński, H. Wincel","doi":"10.1016/0020-7381(83)85036-0","DOIUrl":null,"url":null,"abstract":"<div><p>The gas-phase clustering reactions NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em>−1</sub> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<em>n</em> (<em>n</em> = 1–3) NO<sub>3</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em>−1</sub> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>3</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<em>n</em> (<em>n</em> = 1 and 2) have been studied by means of a high-pressure mass spectrometer at temperatures from 200 to 380 K and at total pressures of 0.5–2 torr. It is demonstrated that under the conditions used here these reactions, with the exception of NO<sub>2</sub><sup>−</sup> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>2</sub><sup>−</sup>· C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>, achieve thermodynamic equilibrium above 1 torr. On the basis of the temperature dependence measurements of the equilibrium constants, thermodynamic data have been determined. The following Δ<em>H</em><sub><em>n</em>−1</sub><sup>0</sup>,<sub><em>n</em></sub> values were obtained: NO<sub>2</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub>; Δ<em>H</em><sub>0,1</sub><sup>0</sup> =−20.9 (indirectly obtained), Δ<em>H</em><sub>1,2</sub><sup>0</sup> = −8.5 and Δ<em>H</em><sub>2,3</sub><sup>0</sup> = −7.3 kcal mol<sup>−1</sup>; NO<sub>2</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub>; Δ<em>H</em><sub>0,1</sub><sup>0</sup> = −17.2 and Δ<em>H</em><sub>1,2</sub><sup>0</sup> = −7.2 kcal mol<sup>−1</sup>.</p><p>Semiempirical INDO MO calculations were performed for NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>0NO<sub>2</sub>)<sub><em>n</em></sub> = <sub>1,2</sub> and NO<sub>3</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub> = <sub>1,2</sub> to test the structures and binding energies of these systems. The experimental observations are discussed in terms of the structure stabilities of the solvated ions.</p></div>","PeriodicalId":13998,"journal":{"name":"International Journal of Mass Spectrometry and Ion Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1983-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-7381(83)85036-0","citationCount":"3","resultStr":"{\"title\":\"Gas-phase solvation of NO2− and NO3− by ethyl nitrate\",\"authors\":\"S. Włodek, Z. Łuczyński, H. Wincel\",\"doi\":\"10.1016/0020-7381(83)85036-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The gas-phase clustering reactions NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em>−1</sub> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<em>n</em> (<em>n</em> = 1–3) NO<sub>3</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em>−1</sub> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>3</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<em>n</em> (<em>n</em> = 1 and 2) have been studied by means of a high-pressure mass spectrometer at temperatures from 200 to 380 K and at total pressures of 0.5–2 torr. It is demonstrated that under the conditions used here these reactions, with the exception of NO<sub>2</sub><sup>−</sup> + C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub> = NO<sub>2</sub><sup>−</sup>· C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>, achieve thermodynamic equilibrium above 1 torr. On the basis of the temperature dependence measurements of the equilibrium constants, thermodynamic data have been determined. The following Δ<em>H</em><sub><em>n</em>−1</sub><sup>0</sup>,<sub><em>n</em></sub> values were obtained: NO<sub>2</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub>; Δ<em>H</em><sub>0,1</sub><sup>0</sup> =−20.9 (indirectly obtained), Δ<em>H</em><sub>1,2</sub><sup>0</sup> = −8.5 and Δ<em>H</em><sub>2,3</sub><sup>0</sup> = −7.3 kcal mol<sup>−1</sup>; NO<sub>2</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub>; Δ<em>H</em><sub>0,1</sub><sup>0</sup> = −17.2 and Δ<em>H</em><sub>1,2</sub><sup>0</sup> = −7.2 kcal mol<sup>−1</sup>.</p><p>Semiempirical INDO MO calculations were performed for NO<sub>2</sub><sup>−</sup>· (C<sub>2</sub>H<sub>5</sub>0NO<sub>2</sub>)<sub><em>n</em></sub> = <sub>1,2</sub> and NO<sub>3</sub><sup>−</sup>·(C<sub>2</sub>H<sub>5</sub>ONO<sub>2</sub>)<sub><em>n</em></sub> = <sub>1,2</sub> to test the structures and binding energies of these systems. The experimental observations are discussed in terms of the structure stabilities of the solvated ions.</p></div>\",\"PeriodicalId\":13998,\"journal\":{\"name\":\"International Journal of Mass Spectrometry and Ion Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1983-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0020-7381(83)85036-0\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Mass Spectrometry and Ion Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0020738183850360\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Mass Spectrometry and Ion Physics","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0020738183850360","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Gas-phase solvation of NO2− and NO3− by ethyl nitrate
The gas-phase clustering reactions NO2−· (C2H5ONO2)n−1 + C2H5ONO2 = NO2−· (C2H5ONO2)n (n = 1–3) NO3−· (C2H5ONO2)n−1 + C2H5ONO2 = NO3−· (C2H5ONO2)n (n = 1 and 2) have been studied by means of a high-pressure mass spectrometer at temperatures from 200 to 380 K and at total pressures of 0.5–2 torr. It is demonstrated that under the conditions used here these reactions, with the exception of NO2− + C2H5ONO2 = NO2−· C2H5ONO2, achieve thermodynamic equilibrium above 1 torr. On the basis of the temperature dependence measurements of the equilibrium constants, thermodynamic data have been determined. The following ΔHn−10,n values were obtained: NO2−·(C2H5ONO2)n; ΔH0,10 =−20.9 (indirectly obtained), ΔH1,20 = −8.5 and ΔH2,30 = −7.3 kcal mol−1; NO2−·(C2H5ONO2)n; ΔH0,10 = −17.2 and ΔH1,20 = −7.2 kcal mol−1.
Semiempirical INDO MO calculations were performed for NO2−· (C2H50NO2)n = 1,2 and NO3−·(C2H5ONO2)n = 1,2 to test the structures and binding energies of these systems. The experimental observations are discussed in terms of the structure stabilities of the solvated ions.