{"title":"高压流动He/O2等离子体中的O2(1Δ)生产:结垢和淬火","authors":"N. Babaeva, M. Kushner, R. A. Arakoni","doi":"10.1063/1.2743878","DOIUrl":null,"url":null,"abstract":"Summary form only given. Chemical oxygen-iodine lasers (COILs) achieve oscillation on the <sup>2</sup>P<sub>1/2</sub>rarr<sup>2</sup>P<sub>3/2</sub> transition of atomic iodine at 1.315 mum by a series of excitation transfers from O<sub>2</sub>(<sup>1</sup>Delta). In electrically excited COILs, (eCOILs) the O<sub>2</sub>(<sup>1</sup>Delta) is produced in a flowing plasma, typically He/O<sub>2</sub>, at a few to tens of Torr. Many svstem issues motivate operating eCOILs at higher pressures to obtain larger absolute densities of O<sub>2</sub>(<sup>1</sup>Delta) for a given yield and provide higher back pressure for expansion. Obtaining high yields of O<sub>2</sub>(<sup>1</sup>Delta) will require careful management of the ozone density [a quencher of O<sub>2</sub>(<sup>1</sup>Delta)], gas temperature and discharge stability. In this paper, we discuss results from a computational investigation of O<sub>2</sub>(<sup>1</sup>Delta) production in flowing plasmas sustained at moderate pressures (< 50-100 Torr). This investigation was conducted using plug-flow and 2-dimensional models. In this study, we scaled power deposition and flow rates such that if there are not second order effects, yield should be constant and absolute O<sub>2</sub>(<sup>1</sup>Delta) production should scale linearly with pressure. We found in many cases that absolute O<sub>2</sub>(<sup>1</sup>Delta) production scaled sub-linearly with pressure. Ground state and vibrationally excited ozone are found to be one of the major quenchers of O<sub>2</sub>(<sup>1</sup>Delta) and the production of O<sub>3</sub> is a sensitive function of pressure. Gas heating per molecule increases at high pressures due to exothermic 3-body reactions which reduces O<sub>3</sub> production, increases O<sub>3</sub> destruction and, for certain conditions, restores yields. With increasing pressure and increasing absolute densities of atomic oxygen and pooling reactions of O<sub>2</sub>(<sup>1</sup>Delta), quenching by these species can become important in the afterglow. The yield of O<sub>2</sub>(<sup>1</sup>Delta) is also determined by discharge stability. For the geometries we investigated, discharge constriction becomes problematic at higher pressures, thereby reducing yields.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"2 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2007-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":"{\"title\":\"O2(1Δ) production in high pressure flowing He/O2 plasmas: scaling and quenching\",\"authors\":\"N. Babaeva, M. Kushner, R. A. Arakoni\",\"doi\":\"10.1063/1.2743878\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Summary form only given. Chemical oxygen-iodine lasers (COILs) achieve oscillation on the <sup>2</sup>P<sub>1/2</sub>rarr<sup>2</sup>P<sub>3/2</sub> transition of atomic iodine at 1.315 mum by a series of excitation transfers from O<sub>2</sub>(<sup>1</sup>Delta). In electrically excited COILs, (eCOILs) the O<sub>2</sub>(<sup>1</sup>Delta) is produced in a flowing plasma, typically He/O<sub>2</sub>, at a few to tens of Torr. Many svstem issues motivate operating eCOILs at higher pressures to obtain larger absolute densities of O<sub>2</sub>(<sup>1</sup>Delta) for a given yield and provide higher back pressure for expansion. Obtaining high yields of O<sub>2</sub>(<sup>1</sup>Delta) will require careful management of the ozone density [a quencher of O<sub>2</sub>(<sup>1</sup>Delta)], gas temperature and discharge stability. In this paper, we discuss results from a computational investigation of O<sub>2</sub>(<sup>1</sup>Delta) production in flowing plasmas sustained at moderate pressures (< 50-100 Torr). This investigation was conducted using plug-flow and 2-dimensional models. In this study, we scaled power deposition and flow rates such that if there are not second order effects, yield should be constant and absolute O<sub>2</sub>(<sup>1</sup>Delta) production should scale linearly with pressure. We found in many cases that absolute O<sub>2</sub>(<sup>1</sup>Delta) production scaled sub-linearly with pressure. Ground state and vibrationally excited ozone are found to be one of the major quenchers of O<sub>2</sub>(<sup>1</sup>Delta) and the production of O<sub>3</sub> is a sensitive function of pressure. Gas heating per molecule increases at high pressures due to exothermic 3-body reactions which reduces O<sub>3</sub> production, increases O<sub>3</sub> destruction and, for certain conditions, restores yields. With increasing pressure and increasing absolute densities of atomic oxygen and pooling reactions of O<sub>2</sub>(<sup>1</sup>Delta), quenching by these species can become important in the afterglow. The yield of O<sub>2</sub>(<sup>1</sup>Delta) is also determined by discharge stability. For the geometries we investigated, discharge constriction becomes problematic at higher pressures, thereby reducing yields.\",\"PeriodicalId\":446230,\"journal\":{\"name\":\"2007 IEEE 34th International Conference on Plasma Science (ICOPS)\",\"volume\":\"2 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2007-06-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2007 IEEE 34th International Conference on Plasma Science (ICOPS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.2743878\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.2743878","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
O2(1Δ) production in high pressure flowing He/O2 plasmas: scaling and quenching
Summary form only given. Chemical oxygen-iodine lasers (COILs) achieve oscillation on the 2P1/2rarr2P3/2 transition of atomic iodine at 1.315 mum by a series of excitation transfers from O2(1Delta). In electrically excited COILs, (eCOILs) the O2(1Delta) is produced in a flowing plasma, typically He/O2, at a few to tens of Torr. Many svstem issues motivate operating eCOILs at higher pressures to obtain larger absolute densities of O2(1Delta) for a given yield and provide higher back pressure for expansion. Obtaining high yields of O2(1Delta) will require careful management of the ozone density [a quencher of O2(1Delta)], gas temperature and discharge stability. In this paper, we discuss results from a computational investigation of O2(1Delta) production in flowing plasmas sustained at moderate pressures (< 50-100 Torr). This investigation was conducted using plug-flow and 2-dimensional models. In this study, we scaled power deposition and flow rates such that if there are not second order effects, yield should be constant and absolute O2(1Delta) production should scale linearly with pressure. We found in many cases that absolute O2(1Delta) production scaled sub-linearly with pressure. Ground state and vibrationally excited ozone are found to be one of the major quenchers of O2(1Delta) and the production of O3 is a sensitive function of pressure. Gas heating per molecule increases at high pressures due to exothermic 3-body reactions which reduces O3 production, increases O3 destruction and, for certain conditions, restores yields. With increasing pressure and increasing absolute densities of atomic oxygen and pooling reactions of O2(1Delta), quenching by these species can become important in the afterglow. The yield of O2(1Delta) is also determined by discharge stability. For the geometries we investigated, discharge constriction becomes problematic at higher pressures, thereby reducing yields.