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    旋转移动床反应器颗粒运动特性数值模拟

    Numerical simulation of particle motion characteristics in rotating moving bed reactor

    • 摘要: 热化学储能技术具有储能密度高、储能时间长、材料成本低、适用温度范围广等优点,在太阳能热储能领域展现出广阔的应用前景。其中,颗粒在反应器内的停留时间与反应转化率、储能效率和系统运行稳定性密切相关。颗粒的停留时间过短,反应转化率较低;颗粒的停留时间过长,储能效率降低,并且材料会出现烧结问题,循环的稳定性降低。为了解决传统的反应器常存在颗粒运动特性不清晰、停留时间难调控等问题,提出了一种新型的内置挡板结构的旋转移动床反应器,适用于聚光太阳能热化学储能。采用离散单元法(Discrete Element Method,DEM)研究了启动阶段和稳态阶段颗粒在反应器内的运动特性,并分析了刮片角度、刮片间距等结构参数以及进料流量和转盘转速等操作参数对停留时间及停留时间方差的影响规律。结果表明:在启动阶段,颗粒在转盘表面进行圆周运动,每旋转一周,刮片就对颗粒施加一次径向推力,使颗粒产生短距离的径向偏移,直至其从转盘边缘离开反应器,启动过程仅需约190 s。在稳态阶段,颗粒在反应器内呈现螺旋运动轨迹,同时伴有轻微的轴向波动;颗粒呈现同心环状波峰波谷分布形貌,并在刮片区域局部堆积,床层厚度为2~3 mm,刮片区域的厚度沿径向逐渐减小,厚度为2~10 mm。颗粒停留时间分布整体呈正态分布,高转速下呈现双峰特性;颗粒的停留时间随刮片角度和间距的增大而增加,随进料流量和转盘转速的增大而减少。通过调整这些参数,可以灵活地控制物料停留时间。在本次研究中,停留时间为 60~120 s,无量纲停留时间方差最小为0.077。

       

      Abstract: Thermochemical energy storage technology has advantages such as high energy storage density, long storage time, low material costs, and a wide applicable temperature range, and demonstrates broad application prospects in the field of solar thermal energy storage. The residence time of particles within the reactor is closely related to reaction conversion rates, energy storage efficiency, and system operational stability. Insufficient residence time results in low reaction conversion rates; conversely, excessive residence time reduces energy storage efficiency and leads to sintering issues in the material, thereby compromising cycle stability. To resolve issues commonly found in traditional reactors, such as unclear particle motion characteristics and difficulty in controlling residence time, a novel rotating moving-bed reactor with an integrated baffle structure is proposed, which is suitable for concentrated solar thermochemical energy storage. The discrete element method (DEM) is employed to investigate the particle motion characteristics within the reactor during both the startup and steady-state phases. The study analyzes the influence of structural parameters (such as baffle angle and baffle spacing) and operational parameters (such as feed flow rate and turntable rotation speed) on residence time and its variance. The results indicate that during the startup phase, the particles undergo circular motion on the surface of the rotating turntable. With each full rotation, the baffles apply a radial pushing force to the particles, causing them to undergo a short-distance radial displacement until they leave the reactor via the edge of the turntable; the startup process takes only about 190 s. During the steady-state phase, the particles exhibit a spiral motion trajectory within the reactor, accompanied by slight axial fluctuations; the particles form a concentric annular distribution pattern with peaks and troughs and accumulate locally in the baffle regions, The bed thickness ranged from 2 to 3 mm, and the thickness of the baffle area gradually decreases radially, ranging from 2 to 10 mm. The particle residence time distribution generally follows a normal distribution and exhibits a bimodal characteristic at high rotational speeds; the residence time increases with increasing baffle angle and spacing, and decreases with increasing feed flow rate and turntable rotational speed. By adjusting and coordinating these parameters, the residence time of the material can be flexibly controlled. In this study, the residence time ranged from approximately 60 to 120 s, with a minimum dimensionless variance of 0.077.

       

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