CN114414959A - A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse - Google Patents

A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse Download PDF

Info

Publication number
CN114414959A
CN114414959A CN202210041020.8A CN202210041020A CN114414959A CN 114414959 A CN114414959 A CN 114414959A CN 202210041020 A CN202210041020 A CN 202210041020A CN 114414959 A CN114414959 A CN 114414959A
Authority
CN
China
Prior art keywords
cable
gaussian pulse
signal
pulse signal
insulation
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN202210041020.8A
Other languages
Chinese (zh)
Inventor
张建文
周围
董海波
题恒
王路伽
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
China University of Mining and Technology CUMT
Original Assignee
China University of Mining and Technology CUMT
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by China University of Mining and Technology CUMT filed Critical China University of Mining and Technology CUMT
Priority to CN202210041020.8A priority Critical patent/CN114414959A/en
Publication of CN114414959A publication Critical patent/CN114414959A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/12Testing dielectric strength or breakdown voltage ; Testing or monitoring effectiveness or level of insulation, e.g. of a cable or of an apparatus, for example using partial discharge measurements; Electrostatic testing

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Relating To Insulation (AREA)

Abstract

The invention discloses a cable evaluation device and method based on a Gaussian pulse two-way propagation coefficient, which comprises a signal generation system, a cable model and a measurement system, wherein the signal generation system comprises a signal generation module, a signal transmission module and a signal transmission module; the pulse signal calibrator is connected with the middle of the cable and is used for generating a Gaussian pulse signal with a certain charge amount; the two ends of the cable are respectively connected with the coaxial cable and connected with an oscilloscope in the measuring system, and Gaussian pulse signals at the first end and the last end of the cable are collected; the oscilloscope in the measuring system is connected with the computer and the network analyzer, and the computer and the network analyzer are used for processing the Gaussian pulse signals at the first end and the last end of the cable so as to obtain the actual propagation coefficient of the Gaussian pulse signals in the cable. And comparing with a theoretical value to obtain the insulation uniform distribution coefficient of the cable, thereby carrying out state evaluation on the cable. The invention obtains the insulation uniform distribution coefficient of the cable based on the propagation coefficient of the Gaussian pulse signal in the cable in two-way transmission, and can effectively evaluate the running state and the insulation aging degree of the cable.

Description

一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse

技术领域technical field

本发明涉及电力电缆状态监测技术领域,具体涉及一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法。The invention relates to the technical field of power cable state monitoring, in particular to a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulses.

背景技术Background technique

电力电缆是电网输送电能的主要设备,电缆供电以其安全可靠、隐蔽耐用、受气候影响小、有利于美化城市布局等优点,特别是随着电缆新技术的使用,使得电缆的成本逐渐下降,获得了越来越广泛的应用。Power cables are the main equipment for power transmission in the power grid. Cable power supply has the advantages of being safe, reliable, concealed and durable, less affected by climate, and conducive to beautifying urban layout. Especially with the use of new cable technologies, the cost of cables has gradually decreased. more and more widely used.

但是,电缆线路在加工时绝缘混入的杂质和气泡、铺设施工中线路弯折都会对电缆的绝缘造成损伤。并且由于电力电缆所处环境非常复杂,长期处于地下阴暗潮湿的环境中,容易造成电缆绝缘的破坏,对输电网络的稳定性和安全性造成影响。由于电力电缆的半导体层与绝缘层会使得高频高斯脉冲信号产生较强的衰减,故可以通过分析高频高斯脉冲信号在电缆中的传输特性来评估电力电缆的运行状态,对于预警电力电缆的故障隐患、提升电力系统的稳定运行能力有着重要意义。However, the impurities and air bubbles mixed in the insulation of the cable line during processing, and the bending of the line during the laying construction will cause damage to the insulation of the cable. And because the environment where the power cable is located is very complex, and it has been in a dark and humid underground environment for a long time, it is easy to cause damage to the cable insulation, which will affect the stability and security of the transmission network. Since the semiconductor layer and insulating layer of the power cable will cause strong attenuation of the high-frequency Gaussian pulse signal, the operation state of the power cable can be evaluated by analyzing the transmission characteristics of the high-frequency Gaussian pulse signal in the cable. It is of great significance to avoid hidden troubles and improve the stable operation ability of the power system.

发明内容SUMMARY OF THE INVENTION

本发明提供一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,结构简单装置可以有效测量高斯脉冲信号在电缆中的实际传播系数,并可由实际传播系数和理论传播系数之比得到电缆的绝缘分布系数,反映电缆的绝缘情况与运行状态,有利于预测其使用寿命。The invention provides a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse. The device with a simple structure can effectively measure the actual propagation coefficient of the Gaussian pulse signal in the cable, and the ratio of the actual propagation coefficient to the theoretical propagation coefficient can be obtained. The insulation distribution coefficient reflects the insulation and operating status of the cable, which is helpful for predicting its service life.

为实现上述目的,一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,包括单芯电缆模型,信号发生系统,还包括测量系统;In order to achieve the above purpose, a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulses, including a single-core cable model, a signal generation system, and a measurement system;

所述单芯电缆模型,信号发生系统和测量系统依次连接;In the single-core cable model, the signal generation system and the measurement system are connected in sequence;

所述单芯电缆模型依次由外到内包括电缆护套,屏蔽层,外半导体层,绝缘层,内半导体层和导体层;The single-core cable model sequentially includes a cable sheath, a shielding layer, an outer semiconductor layer, an insulating layer, an inner semiconductor layer and a conductor layer from outside to inside;

单芯电缆模型的两端分别接同轴电缆,中间接入脉冲信号校准器,首末两端与测量系统中的示波器相连;Both ends of the single-core cable model are connected to coaxial cables respectively, the pulse signal calibrator is connected to the middle, and the first and last ends are connected to the oscilloscope in the measurement system;

所述信号发生系统由一个可以产生高斯脉冲信号的脉冲信号校准器构成,连接在单芯电缆模型的两端;The signal generation system consists of a pulse signal calibrator capable of generating Gaussian pulse signals, which is connected to both ends of the single-core cable model;

所述测量系统由示波器、计算机和网络分析仪组成;The measurement system consists of an oscilloscope, a computer and a network analyzer;

示波器分别与电缆两端相连,采集脉冲信号校准器发出的信号和电缆两端的高斯脉冲信号,并且与同为测量系统的计算机和网络分析仪连接。The oscilloscope is connected to the two ends of the cable, respectively, to collect the signal sent by the pulse signal calibrator and the Gaussian pulse signal at both ends of the cable, and to be connected to the computer and network analyzer that are also measuring systems.

进一步的,电缆中间的脉冲信号校准器可以产生不同电荷量的高斯脉冲信号,其计算公式为:Further, the pulse signal calibrator in the middle of the cable can generate Gaussian pulse signals with different charge amounts, and its calculation formula is:

Figure BDA0003470207440000021
Figure BDA0003470207440000021

其中:U为高斯脉冲信号的峰值电压,r1为导体层(106)半径,r2为绝缘层(104)半径,ε为绝缘材料的介电常数,k为比例系数,取2.82。Where: U is the peak voltage of the Gaussian pulse signal, r 1 is the radius of the conductor layer (106), r 2 is the radius of the insulating layer (104), ε is the dielectric constant of the insulating material, and k is the proportionality coefficient, which is taken as 2.82.

一种基于高斯脉冲双向传播系数的电缆绝缘检测方法,具体包括以下步骤:A cable insulation detection method based on the bidirectional propagation coefficient of Gaussian pulse, which specifically includes the following steps:

启动该系统的脉冲信号校准器,在电缆中间给出一定电荷量的高斯脉冲信号激励,并分别用示波器采集电缆首端和尾端的输出信号。Start the pulse signal calibrator of the system, give Gaussian pulse signal excitation with a certain amount of charge in the middle of the cable, and use the oscilloscope to collect the output signals of the head end and the tail end of the cable respectively.

在采集到输出信号的同时,通过与示波器相连的计算机和网络分析仪将输出信号进行分析与处理。When the output signal is collected, the output signal is analyzed and processed through the computer and network analyzer connected to the oscilloscope.

计算高斯脉冲信号在该电缆中的实际传播系数γ1、γ2,公式为:Calculate the actual propagation coefficients γ 1 , γ 2 of the Gaussian pulse signal in the cable, the formulas are:

Figure BDA0003470207440000031
Figure BDA0003470207440000031

其中:L为电缆长度,Uoj为输出信号,Uin为输入信号。Among them: L is the cable length, U oj is the output signal, U in is the input signal.

进一步的,步骤a中,根据公式

Figure BDA0003470207440000032
确定脉冲信号校准器发出的电荷;Further, in step a, according to the formula
Figure BDA0003470207440000032
Determine the charge emitted by the pulse signal calibrator;

进一步的,步骤b中,将示波器中获取的时域结果用傅里叶变换转化为频域的形式;Further, in step b, the time domain result obtained in the oscilloscope is transformed into the form of the frequency domain by Fourier transform;

进一步的,求解高斯脉冲信号在该电缆中的理论传播系数γ0,确定所述单芯电缆模型的一次参数R、L、C、G:Further, solve the theoretical propagation coefficient γ 0 of the Gaussian pulse signal in the cable, and determine the primary parameters R, L, C, G of the single-core cable model:

弯曲电阻R的求解公式为The formula for solving the bending resistance R is:

Figure BDA0003470207440000033
Figure BDA0003470207440000033

ω=2πfω=2πf

其中:μ0真空磁导率μco为导体的磁导率,σco为导体的电导率,f为信号频率。Among them: μ 0 vacuum permeability μ co is the magnetic permeability of the conductor, σ co is the electrical conductivity of the conductor, and f is the signal frequency.

弯曲电缆电感L的计算方法,公式为:The calculation method of bending cable inductance L, the formula is:

Figure BDA0003470207440000034
Figure BDA0003470207440000034

D=0.916sinθD=0.916sinθ

其中:Rl为圆弧弯曲的半径,θ为与导线长度对应的圆心角。Among them: R l is the radius of arc bending, θ is the central angle corresponding to the length of the wire.

求解弯曲电缆电容C时,需要对内半导体层(105)、绝缘层(104)、外半导体层(103)分别求解,公式为:When solving the bending cable capacitance C, it is necessary to solve the inner semiconductor layer (105), the insulating layer (104), and the outer semiconductor layer (103) respectively, and the formula is:

Figure BDA0003470207440000041
Figure BDA0003470207440000041

其中:εx(ω)为各层介质的介电常数,ε0为真空介电常数。Among them: ε x (ω) is the dielectric constant of each layer of medium, and ε 0 is the vacuum dielectric constant.

由各层的电容值,可求得电缆的电容值,公式为:From the capacitance value of each layer, the capacitance value of the cable can be obtained, and the formula is:

Figure BDA0003470207440000042
Figure BDA0003470207440000042

其中:Csc1为内半导体层(105)的电容,Csc2为外半导体层(103)的电容,Cins为绝缘层(104)的电容。Wherein: C sc1 is the capacitance of the inner semiconductor layer (105), C sc2 is the capacitance of the outer semiconductor layer (103), and C ins is the capacitance of the insulating layer (104).

弯曲电缆电导G的计算公式为:The formula for calculating the conductance G of the curved cable is:

Figure BDA0003470207440000043
Figure BDA0003470207440000043

其中:dsc1为内半导体层(105)厚度,dins为绝缘层(104)厚度,dsc2为外半导体层(103)厚度,σins为绝缘层电导率。Wherein: d sc1 is the thickness of the inner semiconductor layer (105), d ins is the thickness of the insulating layer (104), d sc2 is the thickness of the outer semiconductor layer (103), and σ ins is the conductivity of the insulating layer.

高斯脉冲信号在弯曲电缆中双向传播时的理论传播系数γ0为:The theoretical propagation coefficient γ 0 of the Gaussian pulse signal propagating in both directions in a curved cable is:

Figure BDA0003470207440000044
Figure BDA0003470207440000044

进一步的,计算出电缆的绝缘均匀分布系数Pj,其计算公式为:Further, calculate the insulation uniform distribution coefficient P j of the cable, and its calculation formula is:

Figure BDA0003470207440000045
Figure BDA0003470207440000045

根据绝缘均匀分布系数Pj可评估电缆的绝缘情况与运行状态:当0.9≤Pj≤1.2时,电缆的绝缘情况较好,运行状态稳定;当Pj>1.2或Pj<0.9时,电缆的绝缘老化严重,运行状态不稳定。The insulation condition and operating state of the cable can be evaluated according to the uniform distribution coefficient of insulation P j : when 0.9≤P j ≤1.2, the insulation condition of the cable is good and the operating state is stable; when P j >1.2 or P j <0.9, the cable The insulation aging is serious and the running state is unstable.

与现有技术相比,本文提出的一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,设置了单芯电缆模型,信号发生系统和测量系统,通过脉冲信号校准器发出高斯脉冲信号,模拟电力电缆发生局部放电现象时的运行情况;简化系统的同时,使其更加接近实际工况,保障测量的准确性,通过示波器对单芯电缆两端的信号进行测量,利用PC端对所测得信号进行频域分析,确定其传播系数,并与理论计算值相比较,得出电缆的绝缘均匀分布系数,为评估电缆绝缘性能和老化情况做参考,有利于预测电缆的使用寿命Compared with the prior art, a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse proposed in this paper is set up with a single-core cable model, a signal generation system and a measurement system, and a Gaussian pulse signal is sent out through a pulse signal calibrator. Simulate the operation of the power cable when partial discharge occurs; while simplifying the system, make it closer to the actual working condition to ensure the accuracy of the measurement. The signal is analyzed in the frequency domain to determine its propagation coefficient, and compared with the theoretical calculation value, the uniform distribution coefficient of the cable's insulation is obtained.

附图说明Description of drawings

图1是本发明测量装置的整体分布图;Fig. 1 is the overall distribution diagram of the measuring device of the present invention;

图2是本发明测量方法的流程图;Fig. 2 is the flow chart of the measuring method of the present invention;

图中:In the picture:

1、电力电缆模型,2、信号发生系统,3、测量系统,101、电缆护套,102、屏蔽层,103、外半导体层,104、绝缘层,105、内半导体层,106、导体层,201、脉冲信号校准器,301、示波器,302、网络分析仪,303、计算机1. Power cable model, 2. Signal generation system, 3. Measurement system, 101, Cable sheath, 102, Shielding layer, 103, Outer semiconductor layer, 104, Insulation layer, 105, Inner semiconductor layer, 106, Conductor layer, 201, pulse signal calibrator, 301, oscilloscope, 302, network analyzer, 303, computer

具体实施方式Detailed ways

下面结合附图对本发明作进一步说明The present invention will be further described below in conjunction with the accompanying drawings

如图1所示,一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,包括单芯电缆模型1,信号发生系统2,还包括测量系统3;As shown in FIG. 1 , a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulses includes a single-core cable model 1, a signal generation system 2, and a measurement system 3;

所述单芯电缆模型1,信号发生系统2和测量系统3依次连接.The single-core cable model 1, the signal generation system 2 and the measurement system 3 are connected in sequence.

所述单芯电缆模型依次由外到内包括电缆护套101,屏蔽层102,外半导体层103,绝缘层104,内半导体层105和导体层106。The single-core cable model sequentially includes a cable sheath 101 , a shielding layer 102 , an outer semiconductor layer 103 , an insulating layer 104 , an inner semiconductor layer 105 and a conductor layer 106 from the outside to the inside.

单芯电缆模型1的两端分别接同轴电缆,中间接入脉冲信号校准器201,首末两端分别与测量系统3中的示波器301相连;Both ends of the single-core cable model 1 are respectively connected to coaxial cables, the middle is connected to the pulse signal calibrator 201, and the first and last ends are respectively connected to the oscilloscope 301 in the measurement system 3;

所述信号发生系统由一个可以产生高斯脉冲信号的脉冲信号校准器201构成,连接在单芯电缆模型1的中间;The signal generation system is composed of a pulse signal calibrator 201 capable of generating Gaussian pulse signals, which is connected in the middle of the single-core cable model 1;

所述测量系统3由示波器301、计算机302和网络分析仪303组成;The measurement system 3 consists of an oscilloscope 301, a computer 302 and a network analyzer 303;

示波器301分别与电缆两端相连,采集脉冲信号校准器201发出的信号和电缆两端的高斯脉冲信号,并且与同为测量系统3的计算机302和网络分析仪303连接。The oscilloscope 301 is respectively connected to both ends of the cable, collects the signal sent by the pulse signal calibrator 201 and the Gaussian pulse signal at both ends of the cable, and is connected to the computer 302 and the network analyzer 303 which are also the measurement system 3 .

进一步的,电缆首端的脉冲信号校准器201可以产生不同电荷量的高斯脉冲信号,其计算公式为:Further, the pulse signal calibrator 201 at the head end of the cable can generate Gaussian pulse signals with different charge amounts, and the calculation formula is:

Figure BDA0003470207440000061
Figure BDA0003470207440000061

其中:U为高斯脉冲信号的峰值电压,r1为导体层(106)半径,r2为绝缘层(104)半径,ε为绝缘材料的介电常数,k为比例系数,取2.82。Where: U is the peak voltage of the Gaussian pulse signal, r 1 is the radius of the conductor layer (106), r 2 is the radius of the insulating layer (104), ε is the dielectric constant of the insulating material, and k is the proportionality coefficient, which is taken as 2.82.

一种基于高斯脉冲双向传播系数的电缆绝缘检测方法,具体包括以下步骤:A cable insulation detection method based on the bidirectional propagation coefficient of Gaussian pulse, which specifically includes the following steps:

启动该系统的脉冲信号校准器201,在电缆中间给出一定电荷量的高斯脉冲信号激励,并分别用示波器301采集电缆首端和尾端的输出信号。Start the pulse signal calibrator 201 of the system, give a Gaussian pulse signal excitation with a certain amount of charge in the middle of the cable, and use the oscilloscope 301 to collect the output signals of the head end and the tail end of the cable respectively.

在采集到输出信号的同时,通过与示波器301相连的计算机302和网络分析仪303将输出信号进行分析与处理。When the output signal is collected, the output signal is analyzed and processed through the computer 302 and the network analyzer 303 connected to the oscilloscope 301 .

计算高斯脉冲信号在该电缆中的实际传播系数γ1、γ2,公式为:Calculate the actual propagation coefficients γ 1 , γ 2 of the Gaussian pulse signal in the cable, the formulas are:

Figure BDA0003470207440000071
Figure BDA0003470207440000071

其中:L为电缆长度,Uoj为输出信号,Uin为输入信号。Among them: L is the cable length, U oj is the output signal, U in is the input signal.

进一步的,步骤a中,根据公式

Figure BDA0003470207440000072
确定高斯脉冲信号校验器201发出的电荷Further, in step a, according to the formula
Figure BDA0003470207440000072
Determine the charge from the Gaussian pulse signal checker 201

进一步的,步骤b中,我们将示波器301中获取的时域结果用傅里叶变换转化为频域的形式Further, in step b, we convert the time domain result obtained in the oscilloscope 301 into the form of the frequency domain by Fourier transform

进一步的,求解高斯脉冲信号在该电缆中的理论传播系数γ0,确定所述单芯电缆模型1的一次参数R、L、C、G:Further, solve the theoretical propagation coefficient γ 0 of the Gaussian pulse signal in the cable, and determine the primary parameters R, L, C, G of the single-core cable model 1:

弯曲电阻R的求解公式为The formula for solving the bending resistance R is:

Figure BDA0003470207440000073
Figure BDA0003470207440000073

ω=2πfω=2πf

其中:μ0真空磁导率μco为导体的磁导率,σco为导体的电导率,f为信号频率。Among them: μ 0 vacuum permeability μ co is the magnetic permeability of the conductor, σ co is the electrical conductivity of the conductor, and f is the signal frequency.

弯曲电缆电感L的计算方法,公式为:The calculation method of bending cable inductance L, the formula is:

Figure BDA0003470207440000074
Figure BDA0003470207440000074

D=0.916sinθD=0.916sinθ

其中:Rl为圆弧弯曲的半径,θ为与导线长度对应的圆心角。Among them: R l is the radius of arc bending, θ is the central angle corresponding to the length of the wire.

求解弯曲电缆电容C时,需要对内半导体层(105)、绝缘层(104)、外半导体层(103)分别求解,公式为:When solving the bending cable capacitance C, it is necessary to solve the inner semiconductor layer (105), the insulating layer (104), and the outer semiconductor layer (103) respectively, and the formula is:

Figure BDA0003470207440000075
Figure BDA0003470207440000075

其中:εx(ω)为各层介质的介电常数,ε0为真空介电常数。Among them: ε x (ω) is the dielectric constant of each layer of medium, and ε 0 is the vacuum dielectric constant.

由各层的电容值,可求得电缆的电容值,公式为:From the capacitance value of each layer, the capacitance value of the cable can be obtained, and the formula is:

Figure BDA0003470207440000081
Figure BDA0003470207440000081

其中:Csc1为内半导体层(105)的电容,Csc2为外半导体层(103)的电容,Cins为绝缘层(104)的电容。Wherein: C sc1 is the capacitance of the inner semiconductor layer (105), C sc2 is the capacitance of the outer semiconductor layer (103), and C ins is the capacitance of the insulating layer (104).

弯曲电缆电导G的计算公式为:The formula for calculating the conductance G of the curved cable is:

Figure BDA0003470207440000082
Figure BDA0003470207440000082

其中:dsc1为内半导体层(105)厚度,dins为绝缘层(104)厚度,dsc2为外半导体层(103)厚度,σins为绝缘层电导率。Wherein: d sc1 is the thickness of the inner semiconductor layer (105), d ins is the thickness of the insulating layer (104), d sc2 is the thickness of the outer semiconductor layer (103), and σ ins is the conductivity of the insulating layer.

高斯脉冲信号在弯曲电缆中双向传播时的理论传播系数γ0为:The theoretical propagation coefficient γ 0 of the Gaussian pulse signal propagating in both directions in a curved cable is:

Figure BDA0003470207440000083
Figure BDA0003470207440000083

进一步的,计算出电缆的绝缘均匀分布系数Pj,其计算公式为:Further, calculate the insulation uniform distribution coefficient P j of the cable, and its calculation formula is:

Figure BDA0003470207440000084
Figure BDA0003470207440000084

根据绝缘均匀分布系数Pj可评估电缆的绝缘情况与运行状态:当0.9≤Pj≤1.2时,电缆的绝缘情况较好,运行状态稳定;当Pj>1.2或Pj<0.9时,电缆的绝缘老化严重,运行状态不稳定。The insulation condition and operating state of the cable can be evaluated according to the uniform distribution coefficient of insulation P j : when 0.9≤P j ≤1.2, the insulation condition of the cable is good and the operating state is stable; when P j >1.2 or P j <0.9, the cable The insulation aging is serious and the running state is unstable.

以型号为AXCE-F14/24kV1X150/25LT的电缆为例,电缆长度为10m,电缆护套厚度db=2mm,外半导体层厚度dsc2=0.45mm,绝缘层厚度dins=4.1mm,内半导体层厚度dsc1=0.44mm和导体层半径r1=6.7mm,实验操作方法包括以下步骤:Take the cable model AXCE-F14/24kV1X150/25LT as an example, the cable length is 10m, the cable sheath thickness db = 2mm, the outer semiconductor layer thickness d sc2 = 0.45mm, the insulation layer thickness d ins = 4.1mm, the inner semiconductor layer thickness d sc2 = 0.45mm The layer thickness d sc1 =0.44mm and the conductor layer radius r 1 =6.7mm, the experimental operation method includes the following steps:

1)使用脉冲信号校准器产生100pc电荷量的高斯脉冲信号,其电压幅值为64mv;1) Use the pulse signal calibrator to generate a Gaussian pulse signal with a charge of 100pc, and its voltage amplitude is 64mv;

2)使用示波器采集电缆末端的输出信号,计算机和网络分析仪将输出信号进行傅里叶变换;2) Use the oscilloscope to collect the output signal at the end of the cable, and the computer and the network analyzer will Fourier transform the output signal;

3)通过分析输入信号与输出信号的比值,确定该信号在电缆中的实际传播系数γ1=0.23+j7.3。γ2=0.36+j11.33) By analyzing the ratio of the input signal to the output signal, determine the actual propagation coefficient of the signal in the cable γ 1 =0.23+j7.3. γ 2 =0.36+j11.3

4)对电缆进行建模,求出该电缆的一次参数R、L、C、G,可以求得该信号在电缆中的理论传播系数γ0=0.19+j6.5;4) Model the cable and obtain the primary parameters R, L, C, and G of the cable, and obtain the theoretical propagation coefficient of the signal in the cable γ 0 =0.19+j6.5;

5)根据公式可以求得该电缆的绝缘均匀分布系数P1=1.123,P2=1.738该电缆一端的绝缘情况良好,另一端的绝缘情况较差,需要检修和维护。5) According to the formula, the uniform distribution coefficient of insulation of the cable can be obtained: P 1 =1.123, P 2 =1.738. The insulation of one end of the cable is good, and the insulation of the other end is poor, which needs to be repaired and maintained.

由以上技术方案可知,本发明提供了一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,通过比较高斯脉冲信号在电缆中的理论传播系数与实际传播系数,计算出该电缆的绝缘均匀分布参数,从而评估电缆的绝缘老化程度,有利于预测该电缆的运行状况。在上述实施例中,仅对本发明进行示范性描述,但是本领域技术人员在阅读本专利申请后可以在不脱离本发明的精神和范围的情况下对本发明进行各种修改。It can be seen from the above technical solutions that the present invention provides a cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulses. Distributed parameters to evaluate the insulation aging degree of the cable, which is beneficial to predict the operation status of the cable. In the above-described embodiments, the present invention is only exemplarily described, but those skilled in the art can make various modifications to the present invention without departing from the spirit and scope of the present invention after reading this patent application.

Claims (6)

1.一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,包括单芯电缆模型(1),信号发生系统(2),还包括测量系统(3);1. A cable insulation detection device and method based on a Gaussian pulse bidirectional propagation coefficient, comprising a single-core cable model (1), a signal generation system (2), and a measurement system (3); 所述单芯电缆模型(1),信号发生系统(2)和测量系统(3)依次连接;The single-core cable model (1), the signal generating system (2) and the measuring system (3) are connected in sequence; 所述单芯电缆模型依次由外到内包括电缆护套(101),屏蔽层(102),外半导体层(103),绝缘层(104),内半导体层(105)和导体层(106);The single-core cable model sequentially includes a cable sheath (101), a shielding layer (102), an outer semiconductor layer (103), an insulating layer (104), an inner semiconductor layer (105) and a conductor layer (106) from the outside to the inside ; 单芯电缆模型(1)的两端分别接同轴电缆,首、末两端均与测量系统(3)中的示波器(301)相连;Both ends of the single-core cable model (1) are respectively connected to coaxial cables, and both the first and last ends are connected to the oscilloscope (301) in the measurement system (3); 所述信号发生系统由一个可以产生高斯脉冲信号的脉冲信号校准器(201)构成,连接在单芯电缆模型(1)的中间;The signal generating system consists of a pulse signal calibrator (201) capable of generating Gaussian pulse signals, which is connected in the middle of the single-core cable model (1); 所述测量系统(3)由示波器(301)、计算机(302)和网络分析仪(303)组成;The measurement system (3) consists of an oscilloscope (301), a computer (302) and a network analyzer (303); 示波器(301)分别与电缆两端相连,采集脉冲信号校准器(201)发出的信号和电缆两端的高斯脉冲信号,并且与同为测量系统(3)的计算机(302)和网络分析仪(303)连接。The oscilloscope (301) is respectively connected to both ends of the cable, collects the signal sent by the pulse signal calibrator (201) and the Gaussian pulse signal at both ends of the cable, and communicates with the computer (302) and the network analyzer (303) which are also the measurement system (3). )connect. 2.根据权利要求1所述的一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,其特征在于,电缆首端的脉冲信号校准器(201)可以产生不同电荷量的高斯脉冲信号,其计算公式为:2. a kind of cable insulation detection device and method based on Gaussian pulse bidirectional propagation coefficient according to claim 1, is characterized in that, the pulse signal calibrator (201) of cable head end can produce the Gaussian pulse signal of different charge amounts, its The calculation formula is:
Figure FDA0003470207430000011
Figure FDA0003470207430000011
其中:U为高斯脉冲的峰值电压,r1为导体层(106)半径,r2为绝缘层(104)半径,ε为绝缘材料的介电常数,k为比例系数,取2.82。Where: U is the peak voltage of the Gaussian pulse, r 1 is the radius of the conductor layer (106), r 2 is the radius of the insulating layer (104), ε is the dielectric constant of the insulating material, and k is the proportionality coefficient, which is taken as 2.82.
3.一种基于高斯脉冲双向传播系数的电缆绝缘检测方法,具体包括以下步骤:3. A cable insulation detection method based on the bidirectional propagation coefficient of Gaussian pulse, which specifically comprises the following steps: a.启动该系统的脉冲信号校准器(201),在电缆中间给出一定电荷量的高斯脉冲信号激励,并分别用示波器(301)采集电缆首端和尾端的输出信号;a. Start the pulse signal calibrator (201) of the system, give a Gaussian pulse signal excitation with a certain amount of charge in the middle of the cable, and use the oscilloscope (301) to collect the output signals of the head end and the tail end of the cable respectively; b.在采集到输出信号的同时,通过与示波器(301)相连的计算机(302)和网络分析仪(303)将输出信号进行分析与处理;b. While collecting the output signal, analyze and process the output signal through the computer (302) and the network analyzer (303) connected to the oscilloscope (301); c.计算高斯脉冲信号在该电缆中的实际传播系数γ1、γ2,公式为:c. Calculate the actual propagation coefficients γ 1 , γ 2 of the Gaussian pulse signal in the cable, the formulas are:
Figure FDA0003470207430000021
Figure FDA0003470207430000021
其中:L为电缆长度,Uoj为输出信号,Uin为输入信号。Among them: L is the cable length, U oj is the output signal, U in is the input signal.
4.根据权利要求3所述的一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,其特征在于,步骤a中,根据公式
Figure FDA0003470207430000022
确定高斯脉冲信号校验器(201)发出的电荷;步骤b中,将示波器(301)中获取的时域结果用傅里叶变换转化为频域的形式。
4. a kind of cable insulation detection device and method based on Gaussian pulse bidirectional propagation coefficient according to claim 3, is characterized in that, in step a, according to formula
Figure FDA0003470207430000022
Determine the charge sent by the Gaussian pulse signal checker (201); in step b, convert the time domain result obtained in the oscilloscope (301) into the form of the frequency domain by Fourier transform.
5.根据权利要求1所述的一种基于高斯脉冲双向传播系数的电缆绝缘检测装置及方法,其特征在于,求解高斯脉冲信号在该电缆中的理论传播系数γ0,确定所述单芯电缆模型(1)的一次参数R、L、C、G:5 . The cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse according to claim 1 , wherein the theoretical propagation coefficient γ 0 of the Gaussian pulse signal in the cable is calculated to determine the single-core cable. 6 . The primary parameters R, L, C, G of model (1): 弯曲电阻R的求解公式为The formula for solving the bending resistance R is:
Figure FDA0003470207430000023
Figure FDA0003470207430000023
ω=2πfω=2πf 其中:μ0真空磁导率μco为导体的磁导率,σco为导体的电导率,f为信号频率。Among them: μ 0 vacuum permeability μ co is the magnetic permeability of the conductor, σ co is the electrical conductivity of the conductor, and f is the signal frequency. 弯曲电缆电感L的计算方法,公式为:The calculation method of bending cable inductance L, the formula is:
Figure FDA0003470207430000031
Figure FDA0003470207430000031
D=0.916sinθD=0.916sinθ 其中:Rl为圆弧弯曲的半径;θ为与导线长度对应的圆心角。Among them: R l is the radius of arc bending; θ is the central angle corresponding to the length of the wire. 求解弯曲电缆电容C时,需要对内半导体层(105)、绝缘层(104)、外半导体层(103)分别求解,公式为:When solving the bending cable capacitance C, it is necessary to solve the inner semiconductor layer (105), the insulating layer (104), and the outer semiconductor layer (103) respectively, and the formula is:
Figure FDA0003470207430000032
Figure FDA0003470207430000032
其中:εx(ω)为各层介质的介电常数,ε0为真空介电常数。Among them: ε x (ω) is the dielectric constant of each layer of medium, and ε 0 is the vacuum dielectric constant. 由各层的电容值,可求得电缆的电容值,公式为:From the capacitance value of each layer, the capacitance value of the cable can be obtained, and the formula is:
Figure FDA0003470207430000033
Figure FDA0003470207430000033
其中:Csc1为内半导体层(105)的电容,Csc2为外半导体层(103)的电容,Cins为绝缘层(104)的电容。Wherein: C sc1 is the capacitance of the inner semiconductor layer (105), C sc2 is the capacitance of the outer semiconductor layer (103), and C ins is the capacitance of the insulating layer (104). 弯曲电缆电导G的计算公式为:The formula for calculating the conductance G of the curved cable is:
Figure FDA0003470207430000034
Figure FDA0003470207430000034
其中:dsc1为内半导体层(105)厚度,dins为绝缘层(104)厚度,dsc2为外半导体层(103)厚度,σins为绝缘层电导率。Wherein: d sc1 is the thickness of the inner semiconductor layer (105), d ins is the thickness of the insulating layer (104), d sc2 is the thickness of the outer semiconductor layer (103), and σ ins is the conductivity of the insulating layer. 高斯脉冲信号在弯曲电缆中双向传播时的理论传播系数γ0为:The theoretical propagation coefficient γ 0 of the Gaussian pulse signal propagating in both directions in a curved cable is:
Figure FDA0003470207430000035
Figure FDA0003470207430000035
6.根据权利要求3至5所述的一种基于高斯脉冲信号双向传播系数的电缆评估装置及方法,其特征在于,计算出电缆的绝缘均匀分布系数Pj,其计算公式为:6. a kind of cable evaluation device and method based on Gaussian pulse signal bidirectional propagation coefficient according to claim 3 to 5, is characterized in that, calculates the insulation uniform distribution coefficient P j of cable, its calculation formula is:
Figure FDA0003470207430000041
Figure FDA0003470207430000041
根据绝缘均匀分布系数Pj可评估电缆的绝缘情况与运行状态:当0.9≤Pj≤1.2时,电缆的绝缘情况较好,运行状态稳定;当Pj>1.2或Pj<0.9时,电缆的绝缘老化严重,运行状态不稳定。The insulation condition and operating state of the cable can be evaluated according to the uniform distribution coefficient of insulation P j : when 0.9≤P j ≤1.2, the insulation condition of the cable is good and the operating state is stable; when P j >1.2 or P j <0.9, the cable The insulation aging is serious and the running state is unstable.
CN202210041020.8A 2022-01-14 2022-01-14 A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse Pending CN114414959A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210041020.8A CN114414959A (en) 2022-01-14 2022-01-14 A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210041020.8A CN114414959A (en) 2022-01-14 2022-01-14 A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse

Publications (1)

Publication Number Publication Date
CN114414959A true CN114414959A (en) 2022-04-29

Family

ID=81273999

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210041020.8A Pending CN114414959A (en) 2022-01-14 2022-01-14 A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse

Country Status (1)

Country Link
CN (1) CN114414959A (en)

Similar Documents

Publication Publication Date Title
CN110514959B (en) Positioning method of cable fault FDR positioning system considering cable attenuation characteristics
WO2016019666A1 (en) Method and device for detecting partial discharge of cable
CN113030590B (en) A shielded wire coupling channel high current injection equivalent alternative irradiation test method
CN107942198A (en) A kind of apparatus and method of the cable local defect assessment based on impedance spectrum analysis
CN209590197U (en) A kind of cable fault positioning device based on time-domain pulse reflection method
CN113253046B (en) A method for locating faults in water branches of cables based on impedance spectroscopy
CN113702754A (en) Distribution cable defect positioning algorithm adopting windowed Fourier transform
CN105891761A (en) Scattering parameter-based partial discharge ultrahigh frequency detection system field check method
CN111929532A (en) 10kV distribution cable intermediate joint positioning method
CN114414958A (en) A cable insulation aging assessment device and method based on high frequency signal characteristic impedance
CN110261739B (en) Cable soft fault positioning device and positioning method
CN106324450A (en) Characteristic impedance matching method in cable transmission attenuation characteristic test
CN114966275A (en) Non-intrusive residential load monitoring method and device
CN114414959A (en) A cable insulation detection device and method based on the bidirectional propagation coefficient of Gaussian pulse
CN114414960A (en) A cable evaluation device and method based on two-way propagation coefficient of pulse signal
CN117434386A (en) High-voltage cable sheath defect positioning method based on sheath grounding loop broadband impedance spectrum
CN115128403B (en) A method for measuring online signal of power cable
CN116859182A (en) Method and system for positioning defects of high-voltage cable by considering frequency domain reflection spectrum of cable connector
CN117008012A (en) Short-distance defect detection method and system for instrument control cable
CN115032505A (en) Distribution network cable aging detection and positioning method and system based on broadband impedance spectrum
CN115032497A (en) Cable defect detection system and method based on time-frequency domain reflection
CN118566661A (en) Cable joint insulation assessment device and method
CN106918604A (en) Cable defect detecting system and its detection method based on electromagnetic transmission lineation opinion
CN114152845B (en) Online detection and evaluation method and device for performance of built-in ultrahigh frequency sensor of combined electrical appliance
CN115453213B (en) Electromagnetic shielding effectiveness detection method for aircraft light window based on wave-to-wave converter

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination