Cargando…
Quantitative Measurement of OH* and CH* Chemiluminescence in Jet Diffusion Flames
[Image: see text] Quantitative measurement of chemiluminescence is a challenging work that limits the development of combustion diagnostics based on chemiluminescence. Here, we present a feasible method to obtain effective quantitative chemiluminescence data with an integrating sphere uniform light...
Autores principales: | , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2020
|
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7345390/ https://www.ncbi.nlm.nih.gov/pubmed/32656412 http://dx.doi.org/10.1021/acsomega.0c01093 |
_version_ | 1783556171014078464 |
---|---|
author | Liu, Yao Tan, Jianguo Wan, Minggang Zhang, Lang Yao, Xiao |
author_facet | Liu, Yao Tan, Jianguo Wan, Minggang Zhang, Lang Yao, Xiao |
author_sort | Liu, Yao |
collection | PubMed |
description | [Image: see text] Quantitative measurement of chemiluminescence is a challenging work that limits the development of combustion diagnostics based on chemiluminescence. Here, we present a feasible method to obtain effective quantitative chemiluminescence data with an integrating sphere uniform light source. Spatial distribution images of OH* and CH* radiation from methane laminar diffusion flames were acquired using intensified charge-coupled device (CCD) cameras coupled with multiple lenses and narrow-band-pass filters. After the process of eliminating background emissions by three filters and the Abel inverse transformation, the chemiluminescence intensity was converted to a radiating rate based on the uniform light source. The simulated distributions of OH* and CH* agree well with the experimental results. It has also been found that the distribution of OH* is more extensive and closer to the flame front than that of CH*, demonstrating that OH* is more representative of the flame structure. Based on the change in the reaction rate of different formation reactions, OH* distributions can be divided into three regions: intense section near the nozzle, transition section in the middle of the flame, and secondary section downstream the flame, whereas CH* only exists in the first two regions. In addition, as the velocity ratio of methane and co-flowing air increases, the main reactions become more intense, while the secondary reaction of OH* becomes weaker. |
format | Online Article Text |
id | pubmed-7345390 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-73453902020-07-10 Quantitative Measurement of OH* and CH* Chemiluminescence in Jet Diffusion Flames Liu, Yao Tan, Jianguo Wan, Minggang Zhang, Lang Yao, Xiao ACS Omega [Image: see text] Quantitative measurement of chemiluminescence is a challenging work that limits the development of combustion diagnostics based on chemiluminescence. Here, we present a feasible method to obtain effective quantitative chemiluminescence data with an integrating sphere uniform light source. Spatial distribution images of OH* and CH* radiation from methane laminar diffusion flames were acquired using intensified charge-coupled device (CCD) cameras coupled with multiple lenses and narrow-band-pass filters. After the process of eliminating background emissions by three filters and the Abel inverse transformation, the chemiluminescence intensity was converted to a radiating rate based on the uniform light source. The simulated distributions of OH* and CH* agree well with the experimental results. It has also been found that the distribution of OH* is more extensive and closer to the flame front than that of CH*, demonstrating that OH* is more representative of the flame structure. Based on the change in the reaction rate of different formation reactions, OH* distributions can be divided into three regions: intense section near the nozzle, transition section in the middle of the flame, and secondary section downstream the flame, whereas CH* only exists in the first two regions. In addition, as the velocity ratio of methane and co-flowing air increases, the main reactions become more intense, while the secondary reaction of OH* becomes weaker. American Chemical Society 2020-06-25 /pmc/articles/PMC7345390/ /pubmed/32656412 http://dx.doi.org/10.1021/acsomega.0c01093 Text en Copyright © 2020 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Liu, Yao Tan, Jianguo Wan, Minggang Zhang, Lang Yao, Xiao Quantitative Measurement of OH* and CH* Chemiluminescence in Jet Diffusion Flames |
title | Quantitative Measurement of OH* and CH* Chemiluminescence
in Jet Diffusion Flames |
title_full | Quantitative Measurement of OH* and CH* Chemiluminescence
in Jet Diffusion Flames |
title_fullStr | Quantitative Measurement of OH* and CH* Chemiluminescence
in Jet Diffusion Flames |
title_full_unstemmed | Quantitative Measurement of OH* and CH* Chemiluminescence
in Jet Diffusion Flames |
title_short | Quantitative Measurement of OH* and CH* Chemiluminescence
in Jet Diffusion Flames |
title_sort | quantitative measurement of oh* and ch* chemiluminescence
in jet diffusion flames |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7345390/ https://www.ncbi.nlm.nih.gov/pubmed/32656412 http://dx.doi.org/10.1021/acsomega.0c01093 |
work_keys_str_mv | AT liuyao quantitativemeasurementofohandchchemiluminescenceinjetdiffusionflames AT tanjianguo quantitativemeasurementofohandchchemiluminescenceinjetdiffusionflames AT wanminggang quantitativemeasurementofohandchchemiluminescenceinjetdiffusionflames AT zhanglang quantitativemeasurementofohandchchemiluminescenceinjetdiffusionflames AT yaoxiao quantitativemeasurementofohandchchemiluminescenceinjetdiffusionflames |