生物质燃烧动力学的温度依赖性

H. Saptoadi, T. A. Rohmat, A. Pratoto
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引用次数: 0

摘要

生物质残留物,如稻草,在大多数亚洲国家都是丰富的,在那里大米是可替代的。为了更好地利用废物作为燃料,在其压块之前对其进行热解,以提高热值和碳含量。热解过程在400℃下进行30分钟。热解所需的热量由盘绕在圆柱形反应器周围的电阻镍丝提供。将得到的焦炭粉碎,与天然粘结材料混合,然后压块,形成矩形截面16 × 16 mm,高度28 - 35 mm的棒材。蜂窝煤重约5克,由4克炭和1克粘合剂组成。随后,型煤在同一反应器中进行燃烧过程,但壁温保持350℃不变,燃烧过程的初始温度变化为125℃、150℃、175℃、200℃和225℃。观察到的燃烧过程(由反应速率、燃烧周期和最高温度表示)表明它们与成型煤温度有很强的依赖性,如Arrhenius公式所示。采集的热重数据(温度和质量)被存储和分析,以确定燃烧动力学的活化能和指数前系数。活化能在87 ~ 370 kJ/mol之间变化,指数前系数在195,000 ~ 8.54 × 1035 m/s之间变化更为剧烈。从理论上讲,这些值应该非常相似,因为它们应该是特定于碳的,而不考虑源材料、过程和初始温度。然而,由于固体燃烧是高度不稳定的,所获得的波动数据导致这些不同的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Temperature dependence of biomass combustion kinetics
Biomass residues, such as rice straw, are available abundantly in most Asian countries, where rice is replaceable. In order to better utilize the wastes as fuels, they are pyrolyzed prior to its briquetting in order to improve the Heating Value and carbon content. The pyrolysis process is carried out at 400°C for 30 minutes. The heat required for pyrolysis is supplied by electric resistance nickel wires coiled around the cylindrical reactor. The obtained char is crushed, mixed with natural binding material and then briquetted in form of a bar with rectangular cross sections 16 × 16 mm and height between 28 – 35 mm. The briquettes weigh around 5 gram, consists of 4 gram char and 1 gram binder. Subsequently the briquettes undergo combustion process in the same reactor but the wall temperature is kept constant at 350 °C, while the initial temperature of the combustion process is varied 125 °C, 150 °C, 175 °C, 200 °C, and 225 °C. The observed combustion processes (represented by reaction rates, combustion periods and maximum temperatures) reveal their strong dependence on briquette temperatures, as shown in the Arrhenius formula. The acquired thermogravimetry data (temperatures and masses) are stored and analyzed in order to determine the Activation Energy and Pre-exponential Coefficient of the combustion kinetics. The activation energy varies between 87 and 370 kJ/mol, while the Pre-exponential Coefficient changes even more terribly between 195,000 and 8.54 × 1035 m/s. Theoretically, these values should be closely similar, because they should be specific to carbon, regardless of the source material, the process, and the initial temperature. Nevertheless, since combustion of solids is highly unstable, the acquired fluctuated data lead to these varying results.
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