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首页> 外文期刊>International Journal of Heat and Mass Transfer >Study of wall-to-bed heat transfer in a bubbling fluidised bed using the kinetic theory of granular flow
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Study of wall-to-bed heat transfer in a bubbling fluidised bed using the kinetic theory of granular flow

机译:利用颗粒流动力学理论研究鼓泡流化床中的壁床传热

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摘要

Research into heat transfer modelling in fluidised beds is very limited due to its complexity. The kinetic theory of granular flow (KTGF) has been applied successfully to hydrodynamic modelling in the past but its application in heat transfer modelling has not been tested extensively. A two-fluid Eulerian-Eulerian model has been carried out applying the KTGF to a wall-to-bed reactor. The local heat transfer coefficients are compared against experimental data for two drag models, namely the Gidaspow and the Syamlal-O'Brien drag models. Furthermore, a parametric study is carried out for a variety of coefficients of restitution, particle diameter sizes and inlet velocities. Near wall analysis is carried out in both dense and dilute regions. Both drag models detect the passage of the bubble reasonably well but they predict the complete transition of the bubble past the sensors occurs at slightly different times. The heat transfer coefficients obtained with the Syamlal-O'Brien model showed more local fluctuations than the Gidaspow model because the Syamlal-O'Brien models was developed based on the particle terminal velocities which would indicate a slight sensitivity to a microscopic scale. Extension of the simulation for a longer period makes it possible to reveal that a periodic distribution occurred after 1.5 s and the local heat transfer coefficients gradually reduced to agree better with the experimental results which were previously over estimated. The study shows that a regular dynamic pattern is established in the bubbling fluidised bed only after 1.5-2 s.
机译:由于其复杂性,流化床传热模型的研究非常有限。过去,颗粒流动力学理论(KTGF)已成功地应用于流体动力学建模,但在传热建模中的应用尚未得到广泛的测试。已将KTGF应用于壁床反应器,进行了两种流体的欧拉-欧拉模型。将本地传热系数与两个阻力模型(Gidaspow模型和Syamlal-O'Brien阻力模型)的实验数据进行比较。此外,针对各种恢复系数,粒径大小和入口速度进行了参数研究。在稠密和稀薄区域都进行了近壁分析。两种阻力模型都可以很好地检测到气泡的通过,但它们预测气泡经过传感器的完全过渡发生在略有不同的时间。用Syamlal-O'Brien模型获得的传热系数显示出比Gidaspow模型更大的局部波动,因为Syamlal-O'Brien模型是基于颗粒末端速度开发的,这表明对微观尺度稍有敏感性。延长模拟的时间可以揭示在1.5 s之后出现周期性分布,并且局部传热系数逐渐降低,以更好地与先前过高估计的实验结果相吻合。研究表明,只有在1.5-2 s后,鼓泡流化床才会建立规则的动态模式。

著录项

  • 来源
    《International Journal of Heat and Mass Transfer》 |2010年第22期|p.4949-4959|共11页
  • 作者

    L.M. Armstrong; S. Gu; K.H. Luo;

  • 作者单位

    Energy Technology Research Croup, School of Engineering Sciences, University of Southampton, Southampton, SO17 1BJ, United Kingdom;

    rnEnergy Technology Research Croup, School of Engineering Sciences, University of Southampton, Southampton, SO17 1BJ, United Kingdom;

    rnEnergy Technology Research Croup, School of Engineering Sciences, University of Southampton, Southampton, SO17 1BJ, United Kingdom;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    CFD; heat transfer; fluidised bed; eulerian;

    机译:差价合约传播热量;流化床欧拉;

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