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Three Dimensional CFD-based Numerical Study of Chemical Reacting Char Particles in a Fixed Bed Coal Gasifier

机译:基于三维CFD的固定床煤气化炉中化学反应炭颗粒的数值研究

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摘要

This work is devoted to three-dimensional numerical study of the influence of a hot gas flow and its composition on the carbon consumption evolution within a representative 3D packing of spherical char particles. This field of study is of direct relevance to the understanding of processes inside a fixed bed coal gasifier used for synthesis gas (CO+H_2) production. In particular, the primary interest of this work is the spatial distribution of the temperature and species concentrations in the so-called combustion zone of a fixed bed, where the oxygen reacts with coal particles. In this work the coal-char particles are represented by moisture and ash free nonporous carbon. The model includes six gaseous chemical species (O_2, CO_2, CO, H_2O, H_2, N_2). Three heterogeneous reactions (C+O_2, C+CO_2 and C+H_2O) and two homogeneous semi-global reactions, namely carbon monoxide oxidation and water-gas shift reaction, are employed. The Navier-Stokes equations coupled with the energy and species conservation equations are used to solve the problem in pseudo-steady state approach. At the surface of the particle, the balance of mass, energy and species concentration is applied including the effect of the Stefan flow and the heat loss by radiation at the surface of the particle. The range of parameters considered in this study are d = 2·10~(-2) m, T_(in) = 1000 K, Re = 100, where d, T_(in) and Re are the diameter of the particle, the inlet temperature of the gas and the inlet Reynolds number, respectively. Three different inflow gas compositions arc considered: dry-air case corresponding to Yo_2 =.0.233 and Yh_2o = 0.001, gasification case referring to the gas containing less oxygen with water vapor (Yo_2 = 0.11 ,Yh_2o = 0.074), and finally, a humid-gas case characterized by the following gas composition Yo_2 = 0.11 ,Yh_2o = 0.2. The simulations performed for dry-air case showed the effect of flame penetration into the packing of spherical particles at the inlet Reynolds number of 100. In particular, we found out that the penetration length of the flame is about four particle diameters. Parallel, the analysis of results confirmed that the gas radiation plays a key role for the temperature distribution in the gas phase and on the particle surface, since the mass fractions of water vapor and carbon dioxide are high. In particular, comparative simulations showed that the maximum gas temperature is reduced up to 20% comparing to the case when gas radiation is not taken into account. In the operation of most fixed bed gasifiers it is important to limit the temperature below ash melting point. From this point of view, in this work we studied the influence of different ratios of water vapor to oxygen on the flame extinction and temperature distribution between the particles. Further results are discussed.
机译:这项工作致力于三维数值研究热气流及其组成对球形炭颗粒的代表性3D填充内碳消耗演变的影响。该研究领域与对用于合成气(CO + H_2)生产的固定床煤气化炉内部工艺的理解直接相关。特别地,这项工作的主要兴趣是在所谓的固定床燃烧区中温度和物质浓度的空间分布,在该区域中氧气与煤颗粒反应。在这项工作中,煤焦颗粒由无水分和无灰的无孔碳表示。该模型包括六个气态化学物种(O_2,CO_2,CO,H_2O,H_2,N_2)。使用了三个异质反应(C + O_2,C + CO_2和C + H_2O)和两个均匀的半全局反应,即一氧化碳氧化和水煤气变换反应。 Navier-Stokes方程与能量和物种守恒方程相结合用于解决伪稳态方法中的问题。在粒子的表面施加质量,能量和物质浓度的平衡,包括斯特凡流的影响和粒子表面辐射产生的热损失。本研究中考虑的参数范围是d = 2·10〜(-2)m,T_(in)= 1000 K,Re = 100,其中d,T_(in)和Re是粒子的直径,气体的入口温度和入口的雷诺数。考虑了三种不同的流入气体成分:对应于Yo_2 = .0.233和Yh_2o = 0.001的干燥空气情况,涉及水蒸气中氧气含量较少的气体(Yo_2 = 0.11,Yh_2o = 0.074)的气化情况,最后是潮湿的情况-气体情况,其特征在于以下气体组成Yo_2 = 0.11,Yh_2o = 0.2。在干燥空气情况下进行的模拟显示,在雷诺数为100的入口处,火焰渗透到球形颗粒的填充中。特别是,我们发现火焰的渗透长度约为四个粒径。平行地,结果分析证实,由于水蒸气和二氧化碳的质量分数较高,气体辐射对于气相和颗粒表面的温度分布起关键作用。尤其是,比较模拟显示,与不考虑气体辐射的情况相比,最高气体温度降低了20%。在大多数固定床气化炉的操作中,将温度限制在灰分熔点以下很重要。从这一观点出发,在这项工作中,我们研究了水蒸气与氧气的不同比例对颗粒之间的火焰熄灭和温度分布的影响。讨论了进一步的结果。

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  • 会议地点 Clearwater FL(US);Clearwater FL(US)
  • 作者单位

    CIC Virtuhcon, Department of Energy Process Engineering and Chemical Engineering, Technische Universitaet Bergakademie Freiberg, Fuchsmuhlenweg 9, D-0599 Freiberg, Germany;

    CIC Virtuhcon, Department of Energy Process Engineering and Chemical Engineering, Technische Universitaet Bergakademie Freiberg, Fuchsmuhlenweg 9, D-0599 Freiberg, Germany;

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