{"title":"开发 3.3 μm 附近的盐酸激光吸收诊断仪,用于冲击管化学动力学研究","authors":"Claire M. Grégoire, Eric L. Petersen","doi":"10.1007/s00340-025-08458-3","DOIUrl":null,"url":null,"abstract":"<div><p>A new hydrogen chloride (HCl) laser absorption diagnostic was developed and combined with a shock tube to obtain HCl time-history profiles behind reflected shock waves. An interband cascade laser was used to access the R(8) transition lines of the two isotopes H<sup>35</sup>Cl and H<sup>37</sup>Cl in the fundamental (1 <span>\\(\\leftarrow\\)</span> 0) band at the specific wavelengths of 3045.06 and 3042.74 cm<sup>−1</sup> near 3.3 μm, respectively. Spectroscopic parameters were obtained using HCl in 99.5% Ar, focusing on the line strengths and Ar-broadening effects, and were compared with theory from the literature. Experimental calibration of the HCl absorption coefficient and its dependence over a wide range of temperatures and pressures were obtained (i.e. 1261—1759 K, 0.25—0.42 atm, and 2390—3736 K, 1.26—2.00 atm). Measurements of the line strengths, Ar-broadening parameters at 296 K, and temperature-dependence exponents for the R(8) transition lines of H<sup>35</sup>Cl and H<sup>37</sup>Cl were validated against these results and can be summarized as follows:</p><ol>\n <li>\n <span>1)</span>\n \n <p>For H<sup>35</sup>Cl:<span>\\({S}_{12}\\left({T}_{0}\\right)\\)</span> = 2.099 <span>\\(\\pm\\)</span> 0.084 cm<sup>−2</sup>-atm<sup>−1</sup>, <span>\\({\\gamma }_{H35Cl-Ar}\\left({T}_{0}\\right)\\)</span> = 0.0110 <span>\\(\\pm\\)</span> 0.0005 cm<sup>−1</sup>-atm<sup>−1</sup>, and <span>\\({n}_{H35Cl-Ar}\\)</span> = 0.4 <span>\\(\\pm\\)</span> 0.01.</p>\n \n </li>\n <li>\n <span>2)</span>\n \n <p>For H<sup>37</sup>Cl:<span>\\({S}_{12}\\left({T}_{0}\\right)\\)</span> = 0.708 <span>\\(\\pm\\)</span> 0.028 cm<sup>−2</sup>-atm<sup>−1</sup>, <span>\\({\\gamma }_{H37Cl-Ar}\\left({T}_{0}\\right)\\)</span> = 0.0105 <span>\\(\\pm\\)</span> 0.0005 cm<sup>−1</sup>-atm<sup>−1</sup>, and <span>\\({n}_{H37Cl-Ar}\\)</span> = 0.3 <span>\\(\\pm\\)</span> 0.01.</p>\n \n </li>\n </ol><p>The new HCl laser probe shows promising results for future measurements to better understand the combustion chemistry of propellants containing chlorine.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"131 5","pages":""},"PeriodicalIF":2.0000,"publicationDate":"2025-04-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Development of a HCl laser absorption diagnostic near 3.3 μm for shock-tube chemical kinetics studies\",\"authors\":\"Claire M. Grégoire, Eric L. Petersen\",\"doi\":\"10.1007/s00340-025-08458-3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>A new hydrogen chloride (HCl) laser absorption diagnostic was developed and combined with a shock tube to obtain HCl time-history profiles behind reflected shock waves. An interband cascade laser was used to access the R(8) transition lines of the two isotopes H<sup>35</sup>Cl and H<sup>37</sup>Cl in the fundamental (1 <span>\\\\(\\\\leftarrow\\\\)</span> 0) band at the specific wavelengths of 3045.06 and 3042.74 cm<sup>−1</sup> near 3.3 μm, respectively. Spectroscopic parameters were obtained using HCl in 99.5% Ar, focusing on the line strengths and Ar-broadening effects, and were compared with theory from the literature. Experimental calibration of the HCl absorption coefficient and its dependence over a wide range of temperatures and pressures were obtained (i.e. 1261—1759 K, 0.25—0.42 atm, and 2390—3736 K, 1.26—2.00 atm). Measurements of the line strengths, Ar-broadening parameters at 296 K, and temperature-dependence exponents for the R(8) transition lines of H<sup>35</sup>Cl and H<sup>37</sup>Cl were validated against these results and can be summarized as follows:</p><ol>\\n <li>\\n <span>1)</span>\\n \\n <p>For H<sup>35</sup>Cl:<span>\\\\({S}_{12}\\\\left({T}_{0}\\\\right)\\\\)</span> = 2.099 <span>\\\\(\\\\pm\\\\)</span> 0.084 cm<sup>−2</sup>-atm<sup>−1</sup>, <span>\\\\({\\\\gamma }_{H35Cl-Ar}\\\\left({T}_{0}\\\\right)\\\\)</span> = 0.0110 <span>\\\\(\\\\pm\\\\)</span> 0.0005 cm<sup>−1</sup>-atm<sup>−1</sup>, and <span>\\\\({n}_{H35Cl-Ar}\\\\)</span> = 0.4 <span>\\\\(\\\\pm\\\\)</span> 0.01.</p>\\n \\n </li>\\n <li>\\n <span>2)</span>\\n \\n <p>For H<sup>37</sup>Cl:<span>\\\\({S}_{12}\\\\left({T}_{0}\\\\right)\\\\)</span> = 0.708 <span>\\\\(\\\\pm\\\\)</span> 0.028 cm<sup>−2</sup>-atm<sup>−1</sup>, <span>\\\\({\\\\gamma }_{H37Cl-Ar}\\\\left({T}_{0}\\\\right)\\\\)</span> = 0.0105 <span>\\\\(\\\\pm\\\\)</span> 0.0005 cm<sup>−1</sup>-atm<sup>−1</sup>, and <span>\\\\({n}_{H37Cl-Ar}\\\\)</span> = 0.3 <span>\\\\(\\\\pm\\\\)</span> 0.01.</p>\\n \\n </li>\\n </ol><p>The new HCl laser probe shows promising results for future measurements to better understand the combustion chemistry of propellants containing chlorine.</p></div>\",\"PeriodicalId\":474,\"journal\":{\"name\":\"Applied Physics B\",\"volume\":\"131 5\",\"pages\":\"\"},\"PeriodicalIF\":2.0000,\"publicationDate\":\"2025-04-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Physics B\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s00340-025-08458-3\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Physics B","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1007/s00340-025-08458-3","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"OPTICS","Score":null,"Total":0}
引用次数: 0
摘要
开发了一种新的氯化氢(HCl)激光吸收诊断方法,并将其与激波管相结合,以获得反射激波后的HCl时程分布。利用带间级联激光器分别在3045.06和3042.74 cm−1 (3.3 μm附近)波长处,获取了H35Cl和H37Cl两种同位素基(1 \(\leftarrow\) 0)波段的R(8)过渡谱线。用HCl在99.5溶液中获得光谱参数% Ar, focusing on the line strengths and Ar-broadening effects, and were compared with theory from the literature. Experimental calibration of the HCl absorption coefficient and its dependence over a wide range of temperatures and pressures were obtained (i.e. 1261—1759 K, 0.25—0.42 atm, and 2390—3736 K, 1.26—2.00 atm). Measurements of the line strengths, Ar-broadening parameters at 296 K, and temperature-dependence exponents for the R(8) transition lines of H35Cl and H37Cl were validated against these results and can be summarized as follows: 1) For H35Cl:\({S}_{12}\left({T}_{0}\right)\) = 2.099 \(\pm\) 0.084 cm−2-atm−1, \({\gamma }_{H35Cl-Ar}\left({T}_{0}\right)\) = 0.0110 \(\pm\) 0.0005 cm−1-atm−1, and \({n}_{H35Cl-Ar}\) = 0.4 \(\pm\) 0.01. 2) For H37Cl:\({S}_{12}\left({T}_{0}\right)\) = 0.708 \(\pm\) 0.028 cm−2-atm−1, \({\gamma }_{H37Cl-Ar}\left({T}_{0}\right)\) = 0.0105 \(\pm\) 0.0005 cm−1-atm−1, and \({n}_{H37Cl-Ar}\) = 0.3 \(\pm\) 0.01. The new HCl laser probe shows promising results for future measurements to better understand the combustion chemistry of propellants containing chlorine.
Development of a HCl laser absorption diagnostic near 3.3 μm for shock-tube chemical kinetics studies
A new hydrogen chloride (HCl) laser absorption diagnostic was developed and combined with a shock tube to obtain HCl time-history profiles behind reflected shock waves. An interband cascade laser was used to access the R(8) transition lines of the two isotopes H35Cl and H37Cl in the fundamental (1 \(\leftarrow\) 0) band at the specific wavelengths of 3045.06 and 3042.74 cm−1 near 3.3 μm, respectively. Spectroscopic parameters were obtained using HCl in 99.5% Ar, focusing on the line strengths and Ar-broadening effects, and were compared with theory from the literature. Experimental calibration of the HCl absorption coefficient and its dependence over a wide range of temperatures and pressures were obtained (i.e. 1261—1759 K, 0.25—0.42 atm, and 2390—3736 K, 1.26—2.00 atm). Measurements of the line strengths, Ar-broadening parameters at 296 K, and temperature-dependence exponents for the R(8) transition lines of H35Cl and H37Cl were validated against these results and can be summarized as follows:
1)
For H35Cl:\({S}_{12}\left({T}_{0}\right)\) = 2.099 \(\pm\) 0.084 cm−2-atm−1, \({\gamma }_{H35Cl-Ar}\left({T}_{0}\right)\) = 0.0110 \(\pm\) 0.0005 cm−1-atm−1, and \({n}_{H35Cl-Ar}\) = 0.4 \(\pm\) 0.01.
2)
For H37Cl:\({S}_{12}\left({T}_{0}\right)\) = 0.708 \(\pm\) 0.028 cm−2-atm−1, \({\gamma }_{H37Cl-Ar}\left({T}_{0}\right)\) = 0.0105 \(\pm\) 0.0005 cm−1-atm−1, and \({n}_{H37Cl-Ar}\) = 0.3 \(\pm\) 0.01.
The new HCl laser probe shows promising results for future measurements to better understand the combustion chemistry of propellants containing chlorine.
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