散斑能见度光谱法测量筒仓内颗粒流的颗粒温度

doi:10.11949/0438-1157.20220128

化工学报 ›› 2022, Vol. 73 ›› Issue (6): 2603-2611.DOI: 10.11949/0438-1157.20220128

散斑能见度光谱法测量筒仓内颗粒流的颗粒温度

陈泉¹(),郑泽希²,李然^1,³,孙其诚⁴,杨晖¹()

^1.上海理工大学光电信息与计算机工程学院，上海 200093
^2.上海理工大学机械工程学院，上海 200093
^3.上海理工大学医疗器械与食品学院，上海 200093
^4.清华大学水沙科学与水利水电工程国家重点实验室，北京 100084

收稿日期:2022-01-21 修回日期:2022-04-28 出版日期:2022-06-05 发布日期:2022-06-30
通讯作者: 杨晖
作者简介:陈泉（1990—），男，博士，博士后，chenquan@usst.edu.cn
基金资助:
国家自然科学基金项目(91634202);上海市自然科学基金项目(20ZR1438800);上海市“科技创新行动计划”启明星培育（扬帆专项）项目(22YF1429700)

Measurement of granular temperature during silo flow by speckle visibility spectroscopy

Quan CHEN¹(),Zexi ZHENG²,Ran LI^1,³,Qicheng SUN⁴,Hui YANG¹()

^1.School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
^2.School of Mechanical Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
^3.School of Medical Instrument and Food Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
^4.State Key Laboratory of Hydroscience and Engineering, Tsinghua University, Beijing 100084, China

Received:2022-01-21 Revised:2022-04-28 Online:2022-06-05 Published:2022-06-30
Contact: Hui YANG

摘要/Abstract

摘要：

筒仓内颗粒流在化工生产中广泛应用，准确描述颗粒流的动力学规律对于调控化工反应过程中的混合和传输效率极为重要。颗粒温度是影响颗粒流的重要参数之一，为此搭建了基于线阵CCD相机的散斑能见度光谱测量装置，选取均值粒径分别为0.94和1.55 mm的球形颗粒进行实验。通过测量卸料过程中筒仓内颗粒流的时变颗粒温度，发现了离散颗粒运动在介尺度条件下具有稳定性。进一步，对比两种粒径颗粒的颗粒温度值，观察到稳态流动中大粒径颗粒具有更高的能量耗散，从而建立了宏观质量流率与介观颗粒温度之间的联系。通过分析筒仓内颗粒温度场的分布特征，发现了孔口附近的离散颗粒存在定向有序的运动。最后，根据筒仓内颗粒流堵塞过程中的颗粒温度变化曲线，揭示了颗粒流堵塞的弛豫变化规律。实验结果揭示的筒仓内颗粒流的运动规律，为完善化工生产中颗粒材料的存储与运输提供了参考数据。

关键词: 颗粒流, 动力学, 介尺度, 颗粒温度, 堵塞

Abstract:

Granular flow in silos is widely used in chemical reactions. Accurately grasping the dynamic law of granular flow is extremely important for regulating the mixing and transmission efficiency in chemical reaction process. Granular temperature is one of the important parameters affecting granular flow. In this paper, a speckle visibility spectroscopy measurement device based on linear CCD camera is built, and spherical particles with mean particle sizes of 0.94 and 1.55 mm were selected. By measuring the time-varying granular temperature during silo flow, it was found that the discrete particle motion is stable under mesoscale conditions. Further, comparing the granular temperature values of the two particle sizes, it is observed that the larger particle size has higher energy dissipation in the steady-state flow, so the relationship between the macro mass flow rate and the mesoscopic granular temperature is established. In addition, by analyzing the distribution characteristics of the particle temperature field in the silo, it is found that the discrete particles near the orifice have directional and orderly motion. Finally, according to the curve of granular temperature during the jamming in silos. the relaxation change law of clogging is revealed. The experimental results reveal the law of granular flow in the silo, which provides reference data for improving the storage and transportation of granular material in chemical production.

Key words: granular flow, dynamics, mesoscale, granular temperature, jamming

中图分类号:

TB 133

陈泉, 郑泽希, 李然, 孙其诚, 杨晖. 散斑能见度光谱法测量筒仓内颗粒流的颗粒温度[J]. 化工学报, 2022, 73(6): 2603-2611.

Quan CHEN, Zexi ZHENG, Ran LI, Qicheng SUN, Hui YANG. Measurement of granular temperature during silo flow by speckle visibility spectroscopy[J]. CIESC Journal, 2022, 73(6): 2603-2611.

图/表 9

图1 实验玻璃珠的图片和颗粒粒径的累积分布(fCDF代表颗粒粒径的累积分布函数；d代表颗粒粒径)

Fig.1 The image of glass beads and the cumulative particle size distributions of the glass beads

表1 实验颗粒材料的特征参数

Table 1 Characteristic of granular materials used in this work

材料	密度/(kg/m3)	堆积密度/(kg/m3)	d/mm	β/(°)	静摩擦系数	恢复系数
小玻璃珠	2500	1567±21	0.94±0.06	27.32±0.22	0.52	0.65
大玻璃珠	2500	1428±34	1.55±0.08	25.75±0.16	0.48	0.67

图2 实验装置实物图(D1代表筒仓孔口的长度)

Fig.2 The annotated photo of the experimental setup

图3 散斑能见度光谱法测量颗粒温度的原理示意图[ES (t)代表光程为S的散射光子在t时刻的光强幅值；ki 代表入射激光经过i次散射后的波矢量]

Fig.3 Schematic diagram of measuring granular temperature by speckle visibility spectroscopy

图4 筒仓内颗粒流测量点A(0, 10 mm, 0)的颗粒温度变化曲线(δˉv12代表稳态流中粒径为0.94 mm颗粒的平均颗粒温度；δˉv22代表稳态流中粒径为1.55 mm颗粒的平均颗粒温度)

Fig.4 The curve of granular temperature at measuring point A (0, 10 mm, 0) in silo

表2 统计筒仓内A位置的颗粒温度与质量流率

Table 2 The statistics of the granular temperature on the point A and mass flow rate

参数		1	2	3	4	5	6	7	8	9	10
$δ v 12$ /(mm²/s²)	均值	2.02	2.01	2.02	2.02	2.01	2.03	2.02	2.02	2.03	2.01
$δ v 12$ /(mm²/s²)	方差	0.01	0.02	0.01	0.01	0.01	0.02	0.01	0.03	0.02	0.01
Q₁/(g/s)	均值	32.6	33.5	34.2	33.8	32.2	33.2	33.5	33.8	34.3	32.9
Q₁/(g/s)	方差	0.9	0.5	1.0	0.5	1.0	0.4	0.6	0.4	0.9	0.9
$δ v 22$ /(mm²/s²)	均值	2.32	2.35	2.33	2.37	2.33	2.36	2.32	2.35	2.34	2.36
$δ v 22$ /(mm²/s²)	方差	0.03	0.01	0.02	0.02	0.02	0.02	0.03	0.01	0.02	0.02
Q₂/(g/s)	均值	27.1	26.5	26.9	26.1	27.3	25.9	26.7	27.0	26.5	26.4
Q₂/(g/s)	方差	0.5	0.8	0.7	0.5	0.6	0.6	0.3	0.8	0.4	0.3

表2 统计筒仓内A位置的颗粒温度与质量流率

Table 2 The statistics of the granular temperature on the point A and mass flow rate

参数		1	2	3	4	5	6	7	8	9	10
$δ v 12$ /(mm²/s²)	均值	2.02	2.01	2.02	2.02	2.01	2.03	2.02	2.02	2.03	2.01
$δ v 12$ /(mm²/s²)	方差	0.01	0.02	0.01	0.01	0.01	0.02	0.01	0.03	0.02	0.01
Q₁/(g/s)	均值	32.6	33.5	34.2	33.8	32.2	33.2	33.5	33.8	34.3	32.9
Q₁/(g/s)	方差	0.9	0.5	1.0	0.5	1.0	0.4	0.6	0.4	0.9	0.9
$δ v 22$ /(mm²/s²)	均值	2.32	2.35	2.33	2.37	2.33	2.36	2.32	2.35	2.34	2.36
$δ v 22$ /(mm²/s²)	方差	0.03	0.01	0.02	0.02	0.02	0.02	0.03	0.01	0.02	0.02
Q₂/(g/s)	均值	27.1	26.5	26.9	26.1	27.3	25.9	26.7	27.0	26.5	26.4
Q₂/(g/s)	方差	0.5	0.8	0.7	0.5	0.6	0.6	0.3	0.8	0.4	0.3

图5 稳态流动中筒仓内颗粒流的颗粒温度分布

Fig.5 Granular temperature distribution of steady flow in silo

图6 堵塞过程中均值粒径为0.94 mm颗粒在筒仓内A位置的颗粒温度变化曲线(插图为堵塞前0.06 s时间内的颗粒温度曲线；蓝色实线代表拟合曲线；Δt表示堵塞过程的弛豫时间)

Fig.6 The curve of granular temperature with an average particle size of 0.94 mm at position A in silos during blockage

图7 筒仓内颗粒流堵塞过程的弛豫时间Δt随孔口矩形槽长度D1的变化曲线

Fig.7 The curve of relaxation time of blockage changed with orifice size in silo

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散斑能见度光谱法测量筒仓内颗粒流的颗粒温度

Measurement of granular temperature during silo flow by speckle visibility spectroscopy

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