Spencer C. Barnes, Sean Clees, Joshua A. Vandervort, Taylor M. Rault, Jesse W. Streicher, Christopher L. Strand, Ronald K. Hanson
{"title":"A laser-absorption diagnostic for O2 concentration and temperature using a portable, tunable UV laser system","authors":"Spencer C. Barnes, Sean Clees, Joshua A. Vandervort, Taylor M. Rault, Jesse W. Streicher, Christopher L. Strand, Ronald K. Hanson","doi":"10.1007/s00340-025-08444-9","DOIUrl":null,"url":null,"abstract":"<div><p>A portable ultraviolet (UV) laser absorption diagnostic was developed to measure temperature and O<sub>2</sub> concentration in high-temperature environments. The diagnostic uses two wavelengths (225.0150 nm/44,441.48 cm<sup>−1</sup>; 225.0447 nm/44,435.62 cm<sup>−1</sup>) to probe absorption features with components arising from two different lower vibrational levels of the Schumann–Runge system (<span>\\(B^3 \\Sigma _u^-\\leftarrow X^3 \\Sigma _g^-\\)</span>). To ascertain the position of the features, absorption cross-section measurements were collected at a variety of wavelengths from 225.0000 to 225.0460 nm in a reflected shock tube. After identifying spectral peak locations, the temperature dependence of the absorption cross-section at each peak was measured from 1500 to 5000 K. Experimental measurements motivated changes to an existing spectroscopic model, enabling accurate temperature-dependent cross-section predictions at both wavelengths within experimental uncertainty. Diagnostic validation data shows accurate predictions of temperature and O<sub>2</sub> mole fraction across a wide range of conditions (<i>T</i> = 1600–4500 K; <i>P</i>= 0.15–0.90 atm; <span>\\(\\chi _{O_2}\\)</span> = 2–100%). The average measurement error was 4% for both temperature and mole fraction. The diagnostic was also used to track O<sub>2</sub> dissociation as a function of time behind reflected shock waves and showed good agreement with an in-house coupled vibration-dissociation model.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"131 4","pages":""},"PeriodicalIF":2.0000,"publicationDate":"2025-03-22","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/s00340-025-08444-9","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}
A laser-absorption diagnostic for O2 concentration and temperature using a portable, tunable UV laser system
A portable ultraviolet (UV) laser absorption diagnostic was developed to measure temperature and O2 concentration in high-temperature environments. The diagnostic uses two wavelengths (225.0150 nm/44,441.48 cm−1; 225.0447 nm/44,435.62 cm−1) to probe absorption features with components arising from two different lower vibrational levels of the Schumann–Runge system (\(B^3 \Sigma _u^-\leftarrow X^3 \Sigma _g^-\)). To ascertain the position of the features, absorption cross-section measurements were collected at a variety of wavelengths from 225.0000 to 225.0460 nm in a reflected shock tube. After identifying spectral peak locations, the temperature dependence of the absorption cross-section at each peak was measured from 1500 to 5000 K. Experimental measurements motivated changes to an existing spectroscopic model, enabling accurate temperature-dependent cross-section predictions at both wavelengths within experimental uncertainty. Diagnostic validation data shows accurate predictions of temperature and O2 mole fraction across a wide range of conditions (T = 1600–4500 K; P= 0.15–0.90 atm; \(\chi _{O_2}\) = 2–100%). The average measurement error was 4% for both temperature and mole fraction. The diagnostic was also used to track O2 dissociation as a function of time behind reflected shock waves and showed good agreement with an in-house coupled vibration-dissociation model.
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