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基于双激光雷达的带式输送机煤流量检测系统

于海里 孙立超 左胜 陈大伟 曾祥玉 杜垣江

于海里,孙立超,左胜,等. 基于双激光雷达的带式输送机煤流量检测系统[J]. 工矿自动化,2023,49(7):27-34, 59.  doi: 10.13272/j.issn.1671-251x.2022120004
引用本文: 于海里,孙立超,左胜,等. 基于双激光雷达的带式输送机煤流量检测系统[J]. 工矿自动化,2023,49(7):27-34, 59.  doi: 10.13272/j.issn.1671-251x.2022120004
YU Haili, SUN Lichao, ZUO Sheng, et al. Coal flow detection system for belt conveyor based on dual lidar[J]. Journal of Mine Automation,2023,49(7):27-34, 59.  doi: 10.13272/j.issn.1671-251x.2022120004
Citation: YU Haili, SUN Lichao, ZUO Sheng, et al. Coal flow detection system for belt conveyor based on dual lidar[J]. Journal of Mine Automation,2023,49(7):27-34, 59.  doi: 10.13272/j.issn.1671-251x.2022120004

基于双激光雷达的带式输送机煤流量检测系统

doi: 10.13272/j.issn.1671-251x.2022120004
基金项目: 国家自然科学基金项目(51904142)。
详细信息
    作者简介:

    于海里(1981—),男,内蒙古赤峰人,高级工程师,主要从事露天矿建设和智能化研究工作,E-mail:147218050@qq.com

    通讯作者:

    陈大伟(1980—),男,辽宁凌源人,高级工程师,主要从事矿山智能化工程设计工作,E-mail:13604907048@163.com

  • 中图分类号: TD634.1

Coal flow detection system for belt conveyor based on dual lidar

  • 摘要: 带式输送机煤流运输过程中由于堆积角的存在,使得煤流形状呈近似三角形,易出现检测盲区。针对该问题,提出了一种基于双激光雷达的带式输送机煤流量检测系统。将2个单线激光雷达分别放置在带式输送机上方左右两侧,各测量半个区域内的煤流外轮廓特征点,通过融合算法对左右区域内的煤流外轮廓特征点进行融合,再通过最小二乘多项式拟合算法解算出整个区域内的煤流外轮廓,从而实现对煤流轮廓的无盲区测量。使用光电编码器实时检测输送带运行速度,采用梯形面积累计法计算煤流断面面积,采用面元积分法计算带式输送机的煤流量。现场试验结果表明:无煤料偏置时,单/双激光雷达扫描结果基本一致,系统测量误差为2%~3%,满足煤流量检测要求;有煤料偏置时,基于单激光雷达的系统误差较大,无法满足煤流量检测要求,而基于双激光雷达的系统测量误差依然能够保持在2%~3%。提出了单/双激光雷达选择判据,得出存在煤料偏置或大块煤料的工况下,基于双激光雷达的带式输送机煤流量检测系统更加适用。

     

  • 图  1  基于单激光雷达的煤流量检测系统

    Figure  1.  Coal flow detection system based on single lidar

    图  2  激光雷达检测盲区

    Figure  2.  Blind spot in lidar detection

    图  3  基于双激光雷达的煤流量检测系统

    Figure  3.  Coal flow detection system based on dual lidar

    图  4  带式输送机煤流量检测系统坐标系

    Figure  4.  Coordinate system of coal flow detection system for belt conveyor

    图  5  激光雷达检测盲区判别

    Figure  5.  Identification of blind spot in lidar detection

    图  6  特征点融合流程

    Figure  6.  Feature point fusion process

    图  7  梯形面积累计法原理

    Figure  7.  Principle of trapezoidal area accumulation method

    图  8  煤料瞬时流量计算模型

    Figure  8.  Calculation model for instantaneous coal flow

    图  9  基于双激光雷达的带式输送机煤流量检测系统现场试验

    Figure  9.  Field test of coal flow detection system for belt conveyor based on dual lidar

    图  10  单/双激光雷达扫描结果

    Figure  10.  Single/dual lidar scanning results

    图  11  不同工况下的测量误差

    Figure  11.  Measurement error under different working conditions

    图  12  存在煤料偏置时单激光雷达安装高度

    Figure  12.  Installation height of a single lidar under coal bias condition

    图  13  存在大块煤料时单激光雷达安装高度

    Figure  13.  Installation height of a single lidar in the presence of large blocks of coal

    Step1 分别初始化左右侧激光雷达扫描区间[θ11θ1n]和[θ21θ2n],扫描区间根据激光雷达所在位置和输送带宽度决定;
    Step2for(i=1;ini++)
    Step3读取第i个点的坐标(yizi);
    Step4根据式(5)判别第i个点和第i−1个点Y 轴坐标差值:if |yiyi−1|≥δthen i=0;break;else 将第i 个点的坐标(yizi)存入缓存区 Coordinate_L[ ],Coordinate_R[ ];
    Step5判别第i个点是否超出扫描区间:if θ1iθ1n || θ1iθ11then i=1;break;
    else 对缓存区坐标进行坐标变换,将2个激光雷达的数据转换到同一个坐标系内;
    Step6将缓存区内左右激光雷达坐标变换后的数据按照Y 轴坐标从小到大排序,得到最终的特征点融合数据;
    Step7end
    完成1次数据融合。
    下载: 导出CSV

    表  1  无煤料偏置工况下检测结果对比

    Table  1.   Comparison of detection results under non coal bias working condition

    试验序号带速/
    (m·s−1)
    标准体积/m3检测结果/m3
    单激光
    雷达
    双激光
    雷达
    1221.941.95
    2243.903.88
    3265.855.85
    4287.837.82
    52109.759.73
    6321.961.95
    7343.883.88
    8365.855.86
    9387.807.81
    103109.729.78
    11421.951.95
    12443.903.90
    13465.845.88
    14487.777.83
    154109.749.74
    下载: 导出CSV

    表  2  有煤料偏置工况下检测结果对比

    Table  2.   Comparison of detection results under coal bias working condition

    试验序号带速/
    (m·s−1)
    标准体积/m3测量结果/m3
    单激光
    雷达
    双激光
    雷达
    1221.231.95
    2242.633.90
    3263.785.86
    4285.267.79
    52106.079.72
    6321.351.94
    7342.643.91
    8363.685.86
    9385.017.80
    103106.429.78
    11421.361.95
    12442.653.89
    13463.775.88
    14485.057.78
    154106.439.78
    下载: 导出CSV
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出版历程
  • 收稿日期:  2022-12-01
  • 修回日期:  2023-07-18
  • 网络出版日期:  2023-08-03

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