Measurement of the temperatures of stationary flames

A.G. Loomis, G.St.J. Perrott
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引用次数: 1

Abstract

The concept of temperature as applied to flames is discussed. A number of proposed methods for measuring the temperatures of flames are critically reviewed and the optical method of Kurlbaum-Fery is described and examined in detail. This method depends upon comparing the brightness temperature of a continuous radiator with the brightness of the radiation from the flame colored with an alkali-metal vapor at a given spectral line. From a consideration of the laws of radiation it is shown that the true flame temperature is equal to the brightness temperature of the comparison radiator, as read with an optical pyrometer, when the spectral line is just reversed as seen in a spectrometer.

Curves representing flame temperature as a function of air-gas ratio as measured by the line-reversal method are given for Pittsburgh natural gas, methane, propane, and carbon monoxide. These results are compared with measurements depending on the flame gases heating a solid radiator contained in the flame and with the calculated results for the maximum temperature attainable at complete combustion.

测量静止火焰的温度
讨论了应用于火焰的温度概念。许多提出的测量火焰温度的方法进行了严格审查,并详细描述和检查了克尔鲍姆-费里的光学方法。这种方法依赖于比较连续辐射器的亮度温度与在给定谱线上由碱金属蒸气着色的火焰的辐射亮度。从辐射规律的考虑,表明当光谱线恰好相反时,如在光谱仪中看到的,真实火焰温度等于用光学高温计读出的比较散热器的亮度温度。曲线表示火焰温度作为一个函数的空气-气体比的测量线反转方法给出了匹兹堡天然气,甲烷,丙烷和一氧化碳。这些结果与根据火焰气体加热火焰中包含的固体散热器的测量结果以及完全燃烧时可达到的最高温度的计算结果进行比较。
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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