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架空及埋地多导体线缆对HEMP辐照的瞬态响应

杜子韦华 谢彦召

杜子韦华, 谢彦召. 架空及埋地多导体线缆对HEMP辐照的瞬态响应[J]. 强激光与粒子束, 2019, 31: 070003. doi: 10.11884/HPLPB201931.190142
引用本文: 杜子韦华, 谢彦召. 架空及埋地多导体线缆对HEMP辐照的瞬态响应[J]. 强激光与粒子束, 2019, 31: 070003. doi: 10.11884/HPLPB201931.190142
Du Ziweihua, Xie Yanzhao. Transient response of overhead and buried multiconductor lines to HEMP[J]. High Power Laser and Particle Beams, 2019, 31: 070003. doi: 10.11884/HPLPB201931.190142
Citation: Du Ziweihua, Xie Yanzhao. Transient response of overhead and buried multiconductor lines to HEMP[J]. High Power Laser and Particle Beams, 2019, 31: 070003. doi: 10.11884/HPLPB201931.190142

架空及埋地多导体线缆对HEMP辐照的瞬态响应

doi: 10.11884/HPLPB201931.190142
基金项目: 

西安交通大学电力设备电气绝缘国家重点实验室基金项目 EIPE19114

详细信息
    作者简介:

    杜子韦华(1992-), 女,博士研究生,从事电磁脉冲效应研究;dududzw@126.com

    通讯作者:

    谢彦召(1973-),男,博士,教授,从事电磁脉冲研究;yzxie@xjtu.edu.cn

  • 中图分类号: O441.4

Transient response of overhead and buried multiconductor lines to HEMP

  • 摘要: 针对瞬态电磁场辐照多导体电缆问题,首先介绍了一种用于计算架空及埋地线缆瞬态响应的高效时域宏模型。该模型基于传输线理论,利用广义特征线法和SPICE求解器中集成的模拟行为建模库,在时域内实现建模过程中涉及的频率相关参数和卷积计算。该方法适用性广泛,可同时用于架空及埋地线缆的场线耦合建模仿真;与现有时域有限差分法相比,不需要对时间和空间进行离散,以及对频率相关参数进行矢量匹配或数值逆傅里叶变换,因此可简化建模步骤,提高建模及仿真计算的效率;该宏模型计算效率不受线缆长度限制,适用于研究多导体长距离线缆。其次,在时域和频域分别研究了高空电磁脉冲(HEMP)的环境及特点。最后,利用算例验证了所提宏模型计算架空及埋地线缆响应的有效性,并利用该方法分别研究了架空地线对三相输电线路瞬态响应的影响以及埋地电力电缆金属护套在端接线性及非线性保护器件时对HEMP的瞬态响应。结果表明,宏模型法可在时域内高效地计算入射场耦合架空输电线及埋地电力电缆的瞬态响应,特别是对于带有非线性器件的长多导体线缆。
  • 图  1  外场辐照架空和埋地多导体线缆示意图

    Figure  1.  Geometric configuration for external field coupling to overhead and buried transmission lines

    图  2  多导体埋地电缆等效电路示意图

    Figure  2.  Equivalent circuit of n-conductor underground cables

    图  3  不同土壤电导率和深度处透射电场时域波形

    Figure  3.  Time-domain waveform of transmitted electric field for different ground conductivities and depths

    图  4  不同土壤电导率对应的透射电场幅度谱和归一化累积能流谱

    Figure  4.  Amplitude frequency spectrum and cumulative amount of energy fluence of transmitted electric field for different ground conductivities

    图  5  不同距地面深度对应透射电场的幅度谱和归一化累积能流谱

    Figure  5.  Amplitude frequency spectrum and cumulative amount of energy fluence of transmitted electric field for different depths

    图  6  外场辐照架空线示意图

    Figure  6.  Geometry of transient plane wave coupling to overhead transmission lines

    图  7  负载R1R2R3上感应电压比较

    Figure  7.  Comparing results of induced voltages at the terminal ends obtained via macromodel and BLT in Ref[15]

    图  8  三相输电线和两条地线配置图

    Figure  8.  Configuration of three phase lines and two ground wires

    图  9  外场辐照750 kV三相单回交流输电线路示意图

    Figure  9.  Geometry of plane wave coupling to 750 kV three-phase single-back overhead power lines

    图  10  六分裂导线示意图

    Figure  10.  Geometry of 6-bundle-subconductor transmission line

    图  11  三相感应电压

    Figure  11.  Induced voltages on three phases

    图  12  外场辐照端接接地电阻的单根埋地绝缘电缆示意图

    Figure  12.  Geometry of transient plane wave coupling to a buried insulated cable loaded with grounding resistances

    图  13  不同土壤电导率对应的电缆末端瞬态感应电流比较

    Figure  13.  Comparison of transient induced currents at the far terminal grounding resistive for different ground conductivity

    图  14  三相埋地单芯电缆一端互联经护层过电压保护器接地示意图

    Figure  14.  Configuration of three-phase buried cables connected with sheath protector

    图  15  护套保护器BHQ-8/600的伏安特性

    Figure  15.  V-I characteristic of sheath protector BHQ-8/600

    图  16  电缆金属护层末端感应电压

    Figure  16.  Induced voltages at the end of metallic sheath

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    DL/T401-2002, Guide to the selection of high-voltage cables
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出版历程
  • 收稿日期:  2019-05-05
  • 修回日期:  2019-06-04
  • 刊出日期:  2019-07-15

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