Raman Thermometry of Confined Gas Milli-Flows.

IF 4 3区 综合性期刊 Q2 CHEMISTRY, ANALYTICAL
Sensors Pub Date : 2026-10-08 DOI:10.3390/s26196344
Guzmán Tejeda, Carlos Álvarez, José M Fernández
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Abstract

The temperature of rarefied gas flows inside small channels is hard to measure without disturbing the flow. We present here an optical approach with submillimeter spatial resolution, based on Raman spectroscopy, and several examples of its application to gas flows within millimeter-sized channels. For this work, we have designed and built several channels with different geometries, and forced thermal gradients between some of their surfaces while flowing N2, CO2 and H2 through the channels. The pressures ranged from atmospheric down to 11 mbar, and the flow velocities ranged from 8 to over 450 cm/s. The most rarefied flows lie in the slip regime (Kn ≥0.001). Raman spectra of the flowing gases were recorded inside the channels, and the intensities of the rotational lines were analyzed in terms of Boltzmann plots to retrieve the local gas temperature. It is demonstrated that Raman spectroscopy is able to measure the temperature profiles across dimensions as short as 1 mm inside the channels. The achieved precisions (1-σ uncertainties) at 100 mbar are 0.8 K for CO2, 2.0 K for N2, and 3.7 K for H2.

密闭气体密流的拉曼测温。
稀薄气体在小通道内流动的温度很难在不干扰流动的情况下测量。我们在这里提出了一种基于拉曼光谱的亚毫米空间分辨率的光学方法,以及它在毫米尺寸通道内的气体流动中的几个应用实例。在这项工作中,我们设计并建造了几个不同几何形状的通道,并在它们的一些表面之间施加热梯度,同时通过通道流动N2, CO2和H2。压力范围从大气到11毫巴,流速范围从8到超过450厘米/秒。在滑移区(Kn≥0.001)流动最为稀薄。记录了通道内流动气体的拉曼光谱,并根据玻尔兹曼图分析了旋转线的强度,以获取局部气体温度。结果表明,拉曼光谱能够测量通道内小至1mm的温度分布。在100 mbar下,CO2的精密度为0.8 K, N2的精密度为2.0 K, H2的精密度为3.7 K。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Sensors
Sensors 工程技术-电化学
CiteScore
7.30
自引率
12.80%
发文量
8430
审稿时长
1.7 months
期刊介绍: Sensors (ISSN 1424-8220) provides an advanced forum for the science and technology of sensors and biosensors. It publishes reviews (including comprehensive reviews on the complete sensors products), regular research papers and short notes. Our aim is to encourage scientists to publish their experimental and theoretical results in as much detail as possible. There is no restriction on the length of the papers. The full experimental details must be provided so that the results can be reproduced.
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