Thermocouple error correction for measuring the flame temperature with determination of emissivity and heat transfer coefficient

热电偶 材料科学 发射率 燃烧室 热传导 外推法 机械 传热 传热系数 热力学 温度测量 雷诺数 热辐射 光学 复合材料 燃烧 化学 物理 数学 数学分析 湍流 有机化学
作者
Vijaykumar Hindasageri,R. P. Vedula,S.V. Prabhu
出处
期刊:Review of Scientific Instruments [American Institute of Physics]
卷期号:84 (2) 被引量:125
标识
DOI:10.1063/1.4790471
摘要

Temperature measurement by thermocouples is prone to errors due to conduction and radiation losses and therefore has to be corrected for precise measurement. The temperature dependent emissivity of the thermocouple wires is measured by the use of thermal infrared camera. The measured emissivities are found to be 20%-40% lower than the theoretical values predicted from theory of electromagnetism. A transient technique is employed for finding the heat transfer coefficients for the lead wire and the bead of the thermocouple. This method does not require the data of thermal properties and velocity of the burnt gases. The heat transfer coefficients obtained from the present method have an average deviation of 20% from the available heat transfer correlations in literature for non-reacting convective flow over cylinders and spheres. The parametric study of thermocouple error using the numerical code confirmed the existence of a minimum wire length beyond which the conduction loss is a constant minimal. Temperature of premixed methane-air flames stabilised on 16 mm diameter tube burner is measured by three B-type thermocouples of wire diameters: 0.15 mm, 0.30 mm, and 0.60 mm. The measurements are made at three distances from the burner tip (thermocouple tip to burner tip/burner diameter = 2, 4, and 6) at an equivalence ratio of 1 for the tube Reynolds number varying from 1000 to 2200. These measured flame temperatures are corrected by the present numerical procedure, the multi-element method, and the extrapolation method. The flame temperatures estimated by the two-element method and extrapolation method deviate from numerical results within 2.5% and 4%, respectively.
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