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Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry

Photoacoustic spectroscopy in a differential Helmholtz resonator has been employed with near-IR and red diode lasers for the detection of CO(2), H(2)S and O(2) in 1 bar of air/N(2) and natural gas, in static and flow cell measurements. With the red distributed feedback (DFB) diode laser, O(2) can be...

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Autores principales: Alahmari, Saeed, Kang, Xiu-Wen, Hippler, Michael
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer Berlin Heidelberg 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6595070/
https://www.ncbi.nlm.nih.gov/pubmed/31111181
http://dx.doi.org/10.1007/s00216-019-01877-0
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author Alahmari, Saeed
Kang, Xiu-Wen
Hippler, Michael
author_facet Alahmari, Saeed
Kang, Xiu-Wen
Hippler, Michael
author_sort Alahmari, Saeed
collection PubMed
description Photoacoustic spectroscopy in a differential Helmholtz resonator has been employed with near-IR and red diode lasers for the detection of CO(2), H(2)S and O(2) in 1 bar of air/N(2) and natural gas, in static and flow cell measurements. With the red distributed feedback (DFB) diode laser, O(2) can be detected at 764.3 nm with a noise equivalent detection limit of 0.60 mbar (600 ppmv) in 1 bar of air (35-mW laser, 1-s integration), corresponding to a normalised absorption coefficient α = 2.2 × 10(−8) cm(−1) W s(1/2). Within the tuning range of the near-IR DFB diode laser (6357–6378 cm(−1)), CO(2) and H(2)S absorption features can be accessed, with a noise equivalent detection limit of 0.160 mbar (160 ppmv) CO(2) in 1 bar N(2) (30-mW laser, 1-s integration), corresponding to a normalised absorption coefficient α = 8.3 × 10(−9) cm(−1) W s(1/2). Due to stronger absorptions, the noise equivalent detection limit of H(2)S in 1 bar N(2) is 0.022 mbar (22 ppmv) at 1-s integration time. Similar detection limits apply to trace impurities in 1 bar natural gas. Detection limits scale linearly with laser power and with the square root of integration time. At 16-s total measurement time to obtain a spectrum, a noise equivalent detection limit of 40 ppmv CO(2) is obtained after a spectral line fitting procedure, for example. Possible interferences due to weak water and methane absorptions have been discussed and shown to be either negligible or easy to correct. The setup has been used for simultaneous in situ monitoring of O(2), CO(2) and H(2)S in the cysteine metabolism of microbes (E. coli), and for the analysis of CO(2) and H(2)S impurities in natural gas. Due to the inherent signal amplification and noise cancellation, photoacoustic spectroscopy in a differential Helmholtz resonator has a great potential for trace gas analysis, with possible applications including safety monitoring of toxic gases and applications in the biosciences and for natural gas analysis in petrochemistry. [Figure: see text]
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spelling pubmed-65950702019-07-11 Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry Alahmari, Saeed Kang, Xiu-Wen Hippler, Michael Anal Bioanal Chem Paper in Forefront Photoacoustic spectroscopy in a differential Helmholtz resonator has been employed with near-IR and red diode lasers for the detection of CO(2), H(2)S and O(2) in 1 bar of air/N(2) and natural gas, in static and flow cell measurements. With the red distributed feedback (DFB) diode laser, O(2) can be detected at 764.3 nm with a noise equivalent detection limit of 0.60 mbar (600 ppmv) in 1 bar of air (35-mW laser, 1-s integration), corresponding to a normalised absorption coefficient α = 2.2 × 10(−8) cm(−1) W s(1/2). Within the tuning range of the near-IR DFB diode laser (6357–6378 cm(−1)), CO(2) and H(2)S absorption features can be accessed, with a noise equivalent detection limit of 0.160 mbar (160 ppmv) CO(2) in 1 bar N(2) (30-mW laser, 1-s integration), corresponding to a normalised absorption coefficient α = 8.3 × 10(−9) cm(−1) W s(1/2). Due to stronger absorptions, the noise equivalent detection limit of H(2)S in 1 bar N(2) is 0.022 mbar (22 ppmv) at 1-s integration time. Similar detection limits apply to trace impurities in 1 bar natural gas. Detection limits scale linearly with laser power and with the square root of integration time. At 16-s total measurement time to obtain a spectrum, a noise equivalent detection limit of 40 ppmv CO(2) is obtained after a spectral line fitting procedure, for example. Possible interferences due to weak water and methane absorptions have been discussed and shown to be either negligible or easy to correct. The setup has been used for simultaneous in situ monitoring of O(2), CO(2) and H(2)S in the cysteine metabolism of microbes (E. coli), and for the analysis of CO(2) and H(2)S impurities in natural gas. Due to the inherent signal amplification and noise cancellation, photoacoustic spectroscopy in a differential Helmholtz resonator has a great potential for trace gas analysis, with possible applications including safety monitoring of toxic gases and applications in the biosciences and for natural gas analysis in petrochemistry. [Figure: see text] Springer Berlin Heidelberg 2019-05-20 2019 /pmc/articles/PMC6595070/ /pubmed/31111181 http://dx.doi.org/10.1007/s00216-019-01877-0 Text en © The Author(s) 2019 Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
spellingShingle Paper in Forefront
Alahmari, Saeed
Kang, Xiu-Wen
Hippler, Michael
Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title_full Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title_fullStr Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title_full_unstemmed Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title_short Diode laser photoacoustic spectroscopy of CO(2), H(2)S and O(2) in a differential Helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
title_sort diode laser photoacoustic spectroscopy of co(2), h(2)s and o(2) in a differential helmholtz resonator for trace gas analysis in the biosciences and petrochemistry
topic Paper in Forefront
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6595070/
https://www.ncbi.nlm.nih.gov/pubmed/31111181
http://dx.doi.org/10.1007/s00216-019-01877-0
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