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电动磁浮列车用直线谐波发电机发电特性计算

吕刚 郭曦临

吕刚, 郭曦临. 电动磁浮列车用直线谐波发电机发电特性计算[J]. 西南交通大学学报, 2023, 58(4): 783-791. doi: 10.3969/j.issn.0258-2724.20210892
引用本文: 吕刚, 郭曦临. 电动磁浮列车用直线谐波发电机发电特性计算[J]. 西南交通大学学报, 2023, 58(4): 783-791. doi: 10.3969/j.issn.0258-2724.20210892
LYU Gang, GUO Xilin. Calculation of Power Generation Characteristics of Linear Harmonic Generator for Electrodynamic Suspension Maglev Train[J]. Journal of Southwest Jiaotong University, 2023, 58(4): 783-791. doi: 10.3969/j.issn.0258-2724.20210892
Citation: LYU Gang, GUO Xilin. Calculation of Power Generation Characteristics of Linear Harmonic Generator for Electrodynamic Suspension Maglev Train[J]. Journal of Southwest Jiaotong University, 2023, 58(4): 783-791. doi: 10.3969/j.issn.0258-2724.20210892

电动磁浮列车用直线谐波发电机发电特性计算

doi: 10.3969/j.issn.0258-2724.20210892
基金项目: 国家自然科学基金(52077003,51777009)
详细信息
    作者简介:

    吕刚(1976—),男,教授,博士,研究方向为直线电机及其控制,E-mail:ganglv@bjtu.edu.cn

  • 中图分类号: U266.4

Calculation of Power Generation Characteristics of Linear Harmonic Generator for Electrodynamic Suspension Maglev Train

  • 摘要:

    为研究高速磁悬浮车辆直线谐波发电机的发电特性,首先,基于空间谐波法,提出超导线圈的磁动势分布模型,并推导超导线圈在三维空间内磁感应强度分布公式;其次,基于悬浮线圈与超导线圈间的电磁耦合关系,计算悬浮线圈电流的感应磁场,分析得知悬浮线圈五次谐波磁场用于感应集电;然后,将悬浮线圈五次谐波磁场作为集电线圈的激励,推导集电线圈感应电动势的解析式;最后,以日本山梨线MLX01型磁浮列车为工程背景,利用数值解析值、有限元仿真和日本山梨线实测数据进行了对比分析. 研究结果表明:超导线圈磁感应强度、感应电动势和集电功率的解析值与有限元仿真、实测数据的相对误差均在10%以内,验证了磁动势分布模型和解析模型的有效性;列车速度大于100 km/h时,悬浮线圈电流及其感应磁场趋于饱和;集电线圈感应电动势与列车运行速度近似呈线性关系,集电功率与速度呈二次非线性关系;列车速度500 km/h时,集电功率为43.3 kW;列车速度在380 km/h时达到25.0 kW的目标集电功率,保证了磁悬浮车辆车载供电的可靠性.

     

  • 图 1  直线谐波发电机结构与安装位置

    Figure 1.  Linear harmonic generator structure and installation location

    图 2  直线谐波发电机的线圈排布

    Figure 2.  Coil arrangement of linear harmonic generator

    图 3  超导线圈磁动势分布模型

    Figure 3.  Magnetomotive force distribution model of superconducting coil

    图 4  yOz平面内线圈间位置关系

    Figure 4.  Positional relationship between coils in the yOz plane

    图 5  悬浮线圈电流谐波分析

    Figure 5.  Current harmonic analysis of suspension coil

    图 6  悬浮线圈电流产生的谐波磁场

    Figure 6.  Harmonic magnetic field generated by suspension coil current

    图 7  利用ANSYS 2019 R2建立的三维模型

    Figure 7.  3D model created with ANSYS 2019 R2

    图 8  试验装置

    Figure 8.  Test device

    图 9  超导线圈磁感应强度

    Figure 9.  Magnetic induction intensity of superconducting coil

    图 10  悬浮线圈电流

    Figure 10.  Suspension coil current

    图 11  感应电动势解析计算与有限元仿真对比

    Figure 11.  Comparison between analytical calculation and finite element simulation of induced electromotive force

    图 12  感应电动势解析计算与试验数据对比

    Figure 12.  Comparison between analytical calculation and experimental data of induced electromotive force

    图 13  集电功率解析计算与有限元、试验对比

    Figure 13.  Comparison of collector powers between analytical calculation, finite element simulation and experimental data

    图 14  悬浮线圈电流及其磁感应强度

    Figure 14.  Suspension coil current and its magnetic induction

    图 15  集电线圈感应电动势

    Figure 15.  Induced electromotive force of collector coil

    表  1  直线谐波发电机基本参数

    Table  1.   Parameters of linear harmonic generator

    线圈参数数值
    集电线圈a2R/mm200
    a2S/mm245
    a2T/mm245
    b2U/mm435
    b2B/mm245
    与超导线圈间距/mm75
    悬浮线圈a1/mm350
    b1/mm340
    N1/匝24
    τ1/mm450
    与超导线圈间距/mm185
    超导线圈a0/mm1070
    b0/mm500
    Ns/匝1400
    τ/mm1350
    Is/A500
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出版历程
  • 收稿日期:  2021-11-11
  • 修回日期:  2022-05-10
  • 网络出版日期:  2023-01-07
  • 刊出日期:  2022-05-11

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