<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&#xa0;nm/44,441.48&#xa0;cm<sup>−1</sup>; 225.0447&#xa0;nm/44,435.62&#xa0;cm<sup>−1</sup>) to probe absorption features with components arising from two different lower vibrational levels of the Schumann–Runge system (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="340_2025_8444_Article_IEq4.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="114" /> </InlineMediaObject> <EquationSource Format="TEX">\(B^3 \Sigma _u^-\leftarrow X^3 \Sigma _g^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>B</mi> <mn>3</mn> </msup> <msubsup> <mi mathvariant="normal">Σ</mi> <mi>u</mi> <mo>-</mo> </msubsup> <mo stretchy="false">←</mo> <msup> <mi>X</mi> <mn>3</mn> </msup> <msubsup> <mi mathvariant="normal">Σ</mi> <mi>g</mi> <mo>-</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation>). To ascertain the position of the features, absorption cross-section measurements were collected at a variety of wavelengths from 225.0000 to 225.0460&#xa0;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&#xa0;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&#xa0;K; <i>P</i>= 0.15–0.90&#xa0;atm; <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="340_2025_8444_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(\chi _{O_2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>χ</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> </msub> </math></EquationSource> </InlineEquation> = 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>

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A laser-absorption diagnostic for O2 concentration and temperature using a portable, tunable UV laser system

  • Spencer C. Barnes,
  • Sean Clees,
  • Joshua A. Vandervort,
  • Taylor M. Rault,
  • Jesse W. Streicher,
  • Christopher L. Strand,
  • Ronald K. Hanson

摘要

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 ( \(B^3 \Sigma _u^-\leftarrow X^3 \Sigma _g^-\) B 3 Σ u - X 3 Σ 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; \(\chi _{O_2}\) χ 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.