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Optical Gas-Cell Dynamic Adsorption in a Photoacoustic Spectroscopy-Based SOF(2) and SO(2)F(2) Gas Sensor
SO(2)F(2) and SOF(2) are the main components from the decomposition of insulation gas SF(6). Photoacoustic spectroscopy (PAS) has been acknowledged as an accurate sensing technique. Polar material adsorption for SO(2)F(2) and SOF(2) in the photoacoustic gas cell of PAS may affect detection efficienc...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9611617/ https://www.ncbi.nlm.nih.gov/pubmed/36298300 http://dx.doi.org/10.3390/s22207949 |
Sumario: | SO(2)F(2) and SOF(2) are the main components from the decomposition of insulation gas SF(6). Photoacoustic spectroscopy (PAS) has been acknowledged as an accurate sensing technique. Polar material adsorption for SO(2)F(2) and SOF(2) in the photoacoustic gas cell of PAS may affect detection efficiency. In this paper, the optical gas-cell dynamic adsorptions of four different materials and the detection effects on SO(2)F(2) and SOF(2) are theoretically analyzed and experimentally demonstrated. The materials, including grade 304 stainless steel (SUS304), grade 6061 aluminum alloy (Al6061), polyvinylidene difluoride (PVDC), and polytetrafluoroethylene (PTFE), were applied inside the optical gas cell. The results show that, compared with metallic SUS304 and Al6061, plastic PVDC and PTFE would reduce the gas adsorption of SO(2)F(2) and SOF(2) by 10 to 20% and shorten the response time during gas exchange. The complete gas defusing period in the experiment was about 30 s. The maximum variations of the 90% rising time between the different adsorption materials were approximately 3 s for SO(2)F(2) and 6 s for SOF(2), while the generated photoacoustic magnitudes were identical. This paper explored the material selection for PAS-based gas sensing in practical applications. |
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