4.7 Article

The effect of the photoacoustic Field-Photoacoustic cell coupling term on the performance of the gas detection system

期刊

OPTICS AND LASER TECHNOLOGY
卷 153, 期 -, 页码 -

出版社

ELSEVIER SCI LTD
DOI: 10.1016/j.optlastec.2022.108211

关键词

Gas detection; Photoacoustic spectroscopy; Influencing factors; Coupling term; Optimization

资金

  1. National Natural Science Foundation of China [51607127, 51877157]
  2. Hubei Province Science Fund for Distinguished Young Scholars [2020CFA097]

向作者/读者索取更多资源

The optimization of the photoacoustic cell plays a crucial role in gas detection technology. This study proposes a new factor, the photoacoustic field (PAF)-PAC coupling term, that affects the intensity of PA signals. Through simulation and experiments, it is found that the length and radius of the resonator, as well as the focal length, impact the sound pressure distribution and the light intensity. Additionally, certain distance parameters are related to the optimal response of the gas detection system.
The optimization of the photoacoustic cell (PAC) has always been a research hotspot in the photoacoustic spectroscopy (PAS) based gas detection technology. Herein, a new influential factor of the PA signals intensity, photoacoustic field (PAF)-PAC coupling term was proposed. In addition, the simulation of the sound pressure distribution in the PAC and the PAS gas detection experiment were carried out. The results show that: the length LC and radius RC of the resonator both have an impact on the sound pressure distribution, the strongest sound pressure intensity appears when LC = 95 mm. Besides, when LC is in the range of 35 -65 mm, the sound pressure intensity decreases with the increased RC, whereas it increases with RC when LC is in the range of 80 -125 mm. With the shortening of the focal length F-0, the dimension of the light beam and the maximum light intensity reduces and enhances, respectively. In particular, when F-0 = 16 mm, the integral value along the major axis of the light spot has the peak value, which also changes with the distance l(2) from the laser head to the convex lens, and the peak value appears when l(2) = 4 mm. In addition, the optimal response of the gas detection system (GDS) occurs when l(1) = 0 mm, l(2) = 2 mm, l(3) = 2 mm. LC has a significant impact on the representative signal intensity (RSI), and the influence is mainly result from the PAF-PAC coupling term. However, the effect of the RC on the RSI can be approximately negligible.

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