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Computational Fluid Dynamics (CFD)-Discrete Element Method (DEM) Simulation of Gas-Solid Turbulent Flow in a Cylindrical Spouted Bed with a Conical Base

机译:计算流体动力学(CFD)-离散元方法(DEM)在具有圆锥形基座的圆柱形喷射床中气固湍流的模拟

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摘要

Three dimensionally coupled computational fluid dynamics (CFD) and discrete element method (DEM) were studied for modeling the turbulent gas-solid flow in a cylindrical spouted bed with a conical base. The particle motion was modeled by the DEM, and the gas motion was modeled by the k-e two-equation turbulent model. Drag force, contact force, Saffman lift force, Magnus lift force, and gravitational force acting on an individual particle were considered in establishing the mathematical models. Calculations on the cylindrical spouted bed with an inside diameter of 152 mm, a height of 700 mm, and a conical base of 60° were carried out. Experimental results from the University of British Columbia [He, Y. L.; Qin, S. Z,; Lim, C. J.; Grace, J. R. Particle velocity profiles and solid flow patterns in spouted beds. Can.J. Chem. Eng. 1994, 72 (8), 561 -568] were used as a numerical benchmark to quantitatively assess the simulations. Despite the somewhat larger simulated spout diameter found, the present simulated results were in well-agreement with the experiments. The average error of particle velocity was less than 15%. On the basis of the simulations, the development of spout with time and distributions of particle velocity, particle concentration, and spout diameters at various spouting gas velocities were obtained. Besides, detailed information on particle collision and drag forces adding on particles at different bed regions was discussed. The results showed that particle velocity gradually decreases along the radial direction, with speeds of particles moving upward decreasing with an increasing bed height, while in the annulus region, particles decelerate downward in the cylindrical section and then accelerate in the conical base. The particle concentration increases in the spout region, is kept nearly constant in the annulus region, but decreases in the fountain region along the radial axis. An increasing bed height leads to an increasing particle concentration in the spout region but a decreasing particle concentration in the annulus and fountain regions. Particle collision number, particle turbulent intensity, and the transient collision force and drag force are significantly larger in the spout region than in the annulus and fountain regions. Besides, an increasing spouting gas velocity leads to a remarkable increased speed of particles moving upward or downward, spout diameter, particle collision, drag force, and particle turbulent intensity but decreased particle concentrations.
机译:研究了三维耦合计算流体动力学(CFD)和离散元方法(DEM),以对带有圆锥形底座的圆柱形喷头中的湍流气固流动进行建模。粒子运动由DEM建模,气体运动由k-e二方程湍流模型建模。在建立数学模型时,考虑了作用在单个颗粒上的阻力,接触力,Saffman升力,Magnus升力和重力。对内径为152 mm,高度为700 mm,圆锥形基座为60°的圆柱形喷射床进行了计算。不列颠哥伦比亚大学的实验结果[He,Y. L .;秦世忠; Lim C.J .; Grace,J. R.喷射床中的颗粒速度分布和固体流型。坎·J·化学。 1994,72(8),561 -568]被用作量化评估模拟的数值基准。尽管发现了较大的模拟喷口直径,但目前的模拟结果与实验非常吻合。粒子速度的平均误差小于15%。在模拟的基础上,获得了随时间变化的喷头的发展以及在各种喷头气体速度下的颗粒速度,颗粒浓度和喷头直径的分布。此外,还讨论了有关颗粒碰撞和在不同床层区域添加在颗粒上的阻力的详细信息。结果表明,颗粒速度沿径向方向逐渐减小,向上移动的速度随床高度的增加而减小,而在环形区域,颗粒在圆柱截面中向下减速,然后在圆锥形底部加速。颗粒浓度在喷口区域增加,在环带区域几乎保持恒定,但在喷泉区域沿径向轴减小。床高增加导致喷口区域的颗粒浓度增加,而环空区和喷泉区域的颗粒浓度降低。喷口区域中的粒子碰撞数,粒子湍流强度以及瞬态碰撞力和阻力明显大于环空区和喷泉区。此外,喷射气体速度的增加导致颗粒向上或向下移动的速度显着增加,喷射直径,颗粒碰撞,阻力和颗粒湍流强度,但颗粒浓度降低。

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  • 来源
    《Energy & fuels》 |2011年第sepaaocta期|p.4095-4105|共11页
  • 作者单位

    School of Energy and Environment, Southeast University, Nanjing 210096, People's Republic of China;

    School of Energy and Environment, Southeast University, Nanjing 210096, People's Republic of China;

    School of Energy and Environment, Southeast University, Nanjing 210096, People's Republic of China;

    School of Energy and Environment, Southeast University, Nanjing 210096, People's Republic of China;

    School of Energy and Environment, Southeast University, Nanjing 210096, People's Republic of China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-18 00:41:40

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