CN105842596B - A kind of high sensitivity power cable local defect diagnostic method - Google Patents

A kind of high sensitivity power cable local defect diagnostic method Download PDF

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CN105842596B
CN105842596B CN201610351358.8A CN201610351358A CN105842596B CN 105842596 B CN105842596 B CN 105842596B CN 201610351358 A CN201610351358 A CN 201610351358A CN 105842596 B CN105842596 B CN 105842596B
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power cable
distance
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CN105842596A (en
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周凯
谢敏
赵世林
何珉
张福忠
冉立
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Sichuan University
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    • 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
    • G01R31/1227Testing 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 of components, parts or materials
    • G01R31/1263Testing 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 of components, parts or materials of solid or fluid materials, e.g. insulation films, bulk material; of semiconductors or LV electronic components or parts; of cable, line or wire insulation
    • G01R31/1272Testing 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 of components, parts or materials of solid or fluid materials, e.g. insulation films, bulk material; of semiconductors or LV electronic components or parts; of cable, line or wire insulation of cable, line or wire insulation, e.g. using partial discharge measurements

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Abstract

本发明公开了一种高灵敏度电力电缆局部缺陷诊断方法,该方法基于频域的电力电缆反射系数谱,利用非破坏性试验技术测量分析电力电缆的反射系数谱,结合选通门技术和现代数字信号处理技术实现对电力电缆局部缺陷进行定位,然后通过转换后的反射系数谱的实部或者虚部求得的被测电缆的波速与新电缆的波速进行对比,同时结合转换后的反射系数谱幅值与相应模型拟合曲线的差异,从而实现对局部缺陷的严重程度进行评估。与现有技术相比,本发明不仅能够实现对变化程度较弱的局部缺陷进行定位和多缺陷识别,而且也能够对电力电缆的局部缺陷的严重程度进行评估。

The invention discloses a high-sensitivity power cable local defect diagnosis method. The method is based on the power cable reflection coefficient spectrum in the frequency domain, uses non-destructive test technology to measure and analyze the power cable reflection coefficient spectrum, and combines gate technology and modern digital The signal processing technology realizes the location of local defects in the power cable, and then compares the wave velocity of the tested cable obtained by the real or imaginary part of the converted reflection coefficient spectrum with the wave velocity of the new cable, and combines the converted reflection coefficient spectrum The difference between the amplitude and the corresponding model fitting curve can be used to evaluate the severity of local defects. Compared with the prior art, the present invention can not only realize localization and multi-defect identification of weakly changing local defects, but also evaluate the severity of local defects of the power cable.

Description

一种高灵敏度电力电缆局部缺陷诊断方法A High Sensitivity Diagnosis Method for Local Defects of Power Cables

技术领域technical field

本发明涉及电力电缆运行中的缺陷诊断技术,更为具体地说,是涉及一种电力电缆局部缺陷的诊断方法。The invention relates to defect diagnosis technology during power cable operation, and more specifically relates to a diagnosis method for local defects of power cables.

背景技术Background technique

交联聚乙烯(XLPE)电力电缆因其可靠的电气及机械性能,目前在我国电力工业中得到了广泛的应用。我国在90年代初,开展了大量的城网改造工作,大量的电缆开始应用到城市电网。但是,由于制作工艺以及长期处在不同的运行工况下的影响,电力电缆往往会由于受潮、过热、挤压、弯曲过度等原因造成电力电缆产生水树、绝缘介质变形、铜屏蔽层松动等局部缺陷,如果不对电力电缆的局部缺陷进行处理,电力电缆局部缺陷在强电场的作用下就会迅速发展,最终导致电力电缆绝缘的失效,从而为电力电缆的维护、更换带来大量的工作,导致大量的人力、财力浪费。此外,由于电力电缆埋在地下,并集中在中心城区,对整根电缆进行更换也是一个困难的工作。从节约成本的角度,如果能将电力电缆局部缺陷进行诊断、修复,则可大量节约人力、财力。Cross-linked polyethylene (XLPE) power cables are widely used in my country's electric power industry because of their reliable electrical and mechanical properties. In the early 1990s, my country carried out a large number of urban network transformation work, and a large number of cables began to be applied to urban power grids. However, due to the influence of the manufacturing process and long-term operating conditions, power cables often suffer from moisture, overheating, extrusion, excessive bending, etc., resulting in water trees, deformation of the insulation medium, loose copper shielding, etc. Local defects, if the local defects of the power cable are not dealt with, the local defects of the power cable will develop rapidly under the action of the strong electric field, and eventually lead to the failure of the power cable insulation, thus bringing a lot of work to the maintenance and replacement of the power cable. Result in a lot of manpower and financial waste. In addition, since the power cables are buried underground and concentrated in central urban areas, it is also a difficult job to replace the entire cable. From the perspective of cost saving, if the local defects of power cables can be diagnosed and repaired, a lot of manpower and financial resources can be saved.

现有比较成熟的时域反射法(TDR)能利用脉冲信号实现电力电缆故障的诊断,申请号为201310063871.3,名称为“时域反射系统和方法”的中国发明专利,提供了一种使用时域反射法确定导体异常的方法和系统,但该方法尚无法对变化程度较弱的缺陷进行诊断,并且TDR在多缺陷识别以及近端缺陷识别中的分辨率不够高。电力电缆的局部放电诊断是探测电缆局部缺陷的一种方法,但由于局部放电信号幅值小、衰减严重、信号的分离困难以及多故障识别困难等原因,使得在实际测量中很难实现对局部缺陷进行诊断。同时,局部放电离线测试实验往往是一种破坏性实验,其本身会对电缆的结构产生一定的影响。现有的电力电缆检测诊断技术仍然停留在故障诊断方面,缺乏对电缆结构参数变化程度较弱的局部缺陷进行诊断,无法对电缆的早期缺陷进行排查,因此开展电缆的局部缺陷诊断新技术意义重大。The relatively mature Time Domain Reflectometry (TDR) can use pulse signals to diagnose power cable faults. The application number is 201310063871.3, and the Chinese invention patent named "Time Domain Reflectometry System and Method" provides a method using time domain The reflection method is a method and system for determining conductor abnormalities, but this method is still unable to diagnose defects with a weak degree of change, and the resolution of TDR in multi-defect identification and near-end defect identification is not high enough. Partial discharge diagnosis of power cables is a method to detect local defects of cables, but due to the small amplitude of partial discharge signals, serious attenuation, difficulty in signal separation and difficulty in multi-fault identification, it is difficult to realize partial discharge diagnosis in actual measurement. Defects are diagnosed. At the same time, the partial discharge off-line test experiment is often a destructive experiment, which itself will have a certain impact on the structure of the cable. The existing power cable detection and diagnosis technology still stays in the fault diagnosis, lacks the diagnosis of local defects with weak changes in cable structure parameters, and cannot troubleshoot the early defects of cables. Therefore, it is of great significance to develop new technologies for local defect diagnosis of cables .

发明内容Contents of the invention

本发明的目的是提供一种基于电力电缆反射系数谱的高灵敏度电力电缆局部缺陷诊断方法,实现对电缆的局部缺陷进行精确定位与状态评估,同时也能对电力电缆的中间接头进行很好的区分。具有技术先进、易于操作、成本较低、灵敏度高的优点。The purpose of the present invention is to provide a high-sensitivity power cable local defect diagnosis method based on the power cable reflection coefficient spectrum, which can accurately locate and evaluate the local defects of the cable, and can also perform a good inspection of the middle joint of the power cable. distinguish. It has the advantages of advanced technology, easy operation, low cost and high sensitivity.

本发明提供的高灵敏度电力电缆局部缺陷诊断方法,包括以下步骤:The high-sensitivity power cable local defect diagnosis method provided by the present invention comprises the following steps:

1、待测电缆数据测量1. Data measurement of the cable to be tested

向被测电力电缆发射低压线性调频、伪随机或者高频窄脉冲的信号Vi,测量从电缆末端反射回来的反射信号Vr,通过求出电缆的反射系数谱的幅值|Γd(f)|以及反射系数谱的实部Real(Γd(f))和反射系数谱的虚部Imag(Γd(f)),其中f为信号频率;Transmit a low-voltage linear frequency modulation, pseudo-random or high-frequency narrow pulse signal V i to the power cable under test, measure the reflected signal V r reflected from the end of the cable, and pass Find the amplitude |Γ d (f)| of the reflection coefficient spectrum of the cable and the real part Real(Γ d (f)) of the reflection coefficient spectrum and the imaginary part Imag(Γ d (f)) of the reflection coefficient spectrum, where f is the signal frequency;

2、待测电缆数据处理2. Data processing of the cable to be tested

利用转换函数f→t′,将被测频域信号f转换为t′域信号,然后对转换得到的Real(Γd(t′))或Imag(Γd(t′))进行快速傅里叶(FFT)变换或者离散傅里叶(DFT)变换,记录下能量最大的频率点f0′;然后对转换得到的Real(Γd(t′))或Imag(Γd(t′))与kaiser(凯瑟)窗函数相乘,并进行快速傅里叶变换或者离散傅里叶变换,得到初步处理数据KΓdUsing the conversion function f→t′, the measured frequency domain signal f is converted into a t′ domain signal, and then the converted Real(Γ d (t′)) or Imag(Γ d (t′)) is fast Fourier leaf (FFT) transform or discrete Fourier ( DFT) transform, record the frequency point f 0 ′ with the highest energy; Multiply with the kaiser (Kaiser) window function, and perform fast Fourier transform or discrete Fourier transform to obtain the preliminary processing data KΓd ;

对得到的初步处理数据KΓd做0赫兹至频率点f0′的离散傅里叶变换,将变换结果映射到原始距离诊断图谱D0中,对原始距离诊断图谱D0进行加距离窗处理,得到距离诊断图谱D,其中0赫兹处映射距离为0米,频率点f0′处映射距离为电力电缆长度l;Do the discrete Fourier transform from 0 Hz to the frequency point f 0 ′ on the obtained preliminary processing data KΓ d , map the transformation result to the original distance diagnostic map D 0 , and add a distance window to the original distance diagnostic map D 0 , Obtain the distance diagnostic map D, wherein the mapping distance at 0 Hz is 0 meters, and the mapping distance at the frequency point f 0 ′ is the length l of the power cable;

3、参考电缆数据测量及处理3. Reference cable data measurement and processing

将三相系统中的非被测相电力电缆作为参考电力电缆,然后利用步骤1相同方式求出参考电力电缆的反射系数谱的幅值|Γd1(f)|以及反射系数谱的实部Real(Γd1(f))和反射系数谱的虚部Imag(Γd1(f)),并进行步骤2中相同方式的处理,得到处理后的距离诊断图谱E;Use the non-measured phase power cable in the three-phase system as the reference power cable, and then use the same method as step 1 to find the amplitude |Γ d1 (f)| of the reflection coefficient spectrum of the reference power cable and the real part of the reflection coefficient spectrum Real (Γ d1 (f)) and the imaginary part Imag (Γ d1 (f)) of the reflection coefficient spectrum, and carry out the processing in the same way in step 2, obtain the distance diagnostic map E after processing;

4、电力电缆局部缺陷位置确定4. Determination of the location of local defects in power cables

对比距离诊断图谱D和处理后的距离诊断图谱E,利用选通门技术消除距离诊断图谱D中与处理后的距离诊断图谱E相同位置处的畸变点,得到局部缺陷距离诊断图谱F,从局部缺陷距离诊断图谱F中找到的畸变点,即为电力电缆局部缺陷位置;Comparing the distance diagnostic map D and the processed distance diagnostic map E, using the gate technology to eliminate the distortion points at the same position in the distance diagnostic map D and the processed distance diagnostic map E, to obtain the local defect distance diagnostic map F, from the local The distortion point found in the defect distance diagnostic map F is the local defect position of the power cable;

5、电力电缆局部缺陷判断5. Judgment of local defects of power cables

对得到的局部缺陷距离诊断图谱进行离散傅里叶反变换或快速傅里叶反变换,得到变换后的t′域反射系数谱曲线,并利用转换函数t′→f将t′域反射系数谱转换为Real(Γd2(f))或Imag(Γd2(f)),然后找到Real(Γd2(f))或Imag(Γd2(f))中每个极大值点或极小值点对应的频率fk,利用公式求出被测电力电缆的平均波速,并将vc与同规格的新电力电缆波速v0进行比较,若vc与v0相差1%及以上,说明被测电缆存在局部缺陷,其中N为Real(Γd2)或Imag(Γd2)中极大值点或极小值点的个数。Inverse discrete Fourier transform or inverse fast Fourier transform is performed on the obtained local defect distance diagnostic map to obtain the transformed t′-domain reflection coefficient spectrum curve, and use the conversion function t′→f to convert the t′-domain reflection coefficient spectrum Convert to Real(Γ d2 (f)) or Imag(Γ d2 (f)), and then find each maximum point or minimum value in Real(Γ d2 (f)) or Imag(Γ d2 (f)) The frequency f k corresponding to the point, using the formula Find the average wave velocity of the power cable under test, and compare v c with the wave velocity v 0 of a new power cable of the same specification. If the difference between v c and v 0 is 1% or more, it means that there is a local defect in the test cable, where N is The number of maximum or minimum points in Real(Γ d2 ) or Imag(Γ d2 ).

本发明还可采取下述方法进一步评估被测电力电缆局部缺陷的严重程度:The present invention can also take the following methods to further evaluate the severity of the local defect of the tested power cable:

建立电缆反射系数谱模值数学模型Establishment of Mathematical Model of Spectrum Modulus of Cable Reflection Coefficient

abs(Γd2(f))=a·eb·f+c·ed·f abs(Γ d2 (f))=a·e b·f +c·e d·f

利用建立的数学模型对被测电力电缆测量得到的反射系数谱采用选通门技术后的模值|Γd2(f)|进行数据拟合,求较高频率极值点fk处对应的拟合值,并由下面公式计算得到缺陷程度error进行评估:Use the established mathematical model to perform data fitting on the reflection coefficient spectrum measured by the measured power cable using the gate technology |Γ d2 (f)|, and find the corresponding quasi-parameter at the higher frequency extreme point f k Combined value, and the defect degree error calculated by the following formula for evaluation:

error=std((|Γd2(fk)|-abs(Γd2(fk)))/abs(Γd2(fk)))×100%error=std((|Γ d2 (f k )|-abs(Γ d2 (f k )))/abs(Γ d2 (f k )))×100%

当error<5%时,电缆局部缺陷较轻,此时被测电力电缆可能存在少量铜屏蔽层松动缺陷或者绝缘介质存在刀痕划伤等缺陷;当5%≤error≤10%时,电力电缆缺陷程度中等,此时被测电力电缆可能存在绝缘介质受潮或大面积铜屏蔽层破损等缺陷;当error>10%时,电缆缺陷非常严重,此时被测电力电缆可能存在绝缘介质严重变形等缺陷。公式中的std为标准差。When the error<5%, the partial defect of the cable is relatively light. At this time, the power cable under test may have a small amount of loose copper shielding layer or the insulation medium has defects such as knife marks and scratches; when 5%≤error≤10%, the power cable The degree of defect is moderate. At this time, the power cable under test may have defects such as damp insulation medium or large-area copper shielding layer damage. When error>10%, the cable defect is very serious. At this time, the power cable under test may have severe deformation of the insulation medium, etc. defect. The std in the formula is the standard deviation.

在本发明的上述技术方案中,所述kaiser窗函数中的β取值应满足:In the above-mentioned technical scheme of the present invention, the β value in the described kaiser window function should satisfy:

其中α为旁瓣衰减倍数。Where α is the side lobe attenuation multiple.

在本发明的上述技术方案中,原始距离诊断图谱D0优先采用下述公式进行加距离窗处理:In the above-mentioned technical scheme of the present invention, the original distance diagnostic atlas D 0 preferably adopts the following formula to add distance window processing:

其中s为窗口长度,取值不大于距离诊断图谱D0中的空间分辨率,D为处理后得到的距离诊断图谱。Where s is the window length, and the value is not greater than the spatial resolution in the distance diagnostic atlas D 0 , and D is the distance diagnostic atlas obtained after processing.

在本发明的上述技术方案中,步骤5中所述同规格新电缆的波速v0可由公式计算获得,其中L和C分别为同规格新电缆单位长度的电感和电容;也可采用时域反射法测取获得。In the above-mentioned technical scheme of the present invention, described in the step 5 with the wave velocity v of the new cable of specification can be by formula Obtained by calculation, where L and C are the inductance and capacitance per unit length of a new cable of the same specification; it can also be obtained by time domain reflection method.

由于测量过程中电力电缆中间接头位置也会出现畸变点,影响缺陷位置的判断,为了消除电力电缆的中间接头对缺陷位置判断的影响,本发明在诊断方法步骤3中引入了参考电力电缆进行对比,即将三相系统中的非被测相电力电缆作为参考电力电缆,然后利用步骤1相同方式求出参考电力电缆的反射系数谱的幅值|Γd1(f)|以及反射系数谱的实部Real(Γd1(f))和反射系数谱的虚部Imag(Γd1(f)),并进行步骤2中相同方式的处理,得到处理后的距离诊断图谱E。Since the position of the middle joint of the power cable will also have distortion points during the measurement process, which will affect the judgment of the defect position, in order to eliminate the influence of the middle joint of the power cable on the judgment of the defect position, the present invention introduces a reference power cable for comparison in step 3 of the diagnosis method , that is, the non-measured phase power cable in the three-phase system is used as the reference power cable, and then the amplitude |Γ d1 (f)| of the reflection coefficient spectrum of the reference power cable and the real part of the reflection coefficient spectrum Real(Γ d1 (f)) and the imaginary part Imag(Γ d1 (f)) of the reflection coefficient spectrum, and perform the same processing in step 2 to obtain the processed distance diagnostic map E.

由于通常情况下电力电缆的每一相都会在相同位置制作中间接头,为了消除中间接头对电缆局部缺陷位置判断的影响,本发明在诊断方法步骤4中,采用了对比距离诊断图谱D和距离诊断图谱E的方法,利用选通门技术消除距离诊断图谱D中与距离诊断图谱E相同位置处的畸变点,得到局部缺陷距离诊断图谱F,从局部缺陷距离诊断图谱F中找到的畸变点,畸变点就是局部缺陷位置。Usually, each phase of the power cable will make an intermediate joint at the same position, in order to eliminate the impact of the intermediate joint on the judgment of the local defect position of the cable, in step 4 of the diagnostic method, the present invention adopts a comparison distance diagnosis map D and a distance diagnosis The method of map E uses the gate technology to eliminate the distortion points at the same position in the distance diagnostic map D as the distance diagnostic map E, and obtains the local defect distance diagnostic map F, the distortion points found from the local defect distance diagnostic map F, the distortion The point is the local defect location.

在电力电缆局部缺陷诊断中,存在电力电缆长,信号衰减严重,所需的信号频带较窄;电力电缆短,信号衰减较小,所需的信号频带较宽。同时当信号未衰减为零时,信号的频带越宽,定位精度与灵敏度都越高。In the local defect diagnosis of power cables, there are long power cables, severe signal attenuation, and a narrow signal frequency band required; short power cables, small signal attenuation, and a wide signal frequency band required. At the same time, when the signal is not attenuated to zero, the wider the frequency band of the signal, the higher the positioning accuracy and sensitivity.

本发明提供的电力电缆局部缺陷诊断方法,具有如下十分突出的优点和有益技术效果:The method for diagnosing local defects of power cables provided by the present invention has the following outstanding advantages and beneficial technical effects:

1.本发明的缺陷诊断方法采用的是低压测量方式而非破坏式试验测量方式,不仅不会对电缆绝缘造成损伤,还可减小测量设备的重量和体积。1. The defect diagnosis method of the present invention adopts a low-voltage measurement method instead of a destructive test measurement method, which not only does not cause damage to the cable insulation, but also reduces the weight and volume of the measurement equipment.

2.本发明利用对频域信息进行处理的方式使电缆局部缺陷更容易表现出来,在此基础上通过与kaiser窗函数的结合,大大提高了对电缆局部缺陷定位的灵敏度。2. The present invention uses the method of processing frequency domain information to make local cable defects easier to display, and on this basis, through the combination with Kaiser window function, the sensitivity of local cable defect location is greatly improved.

3.相比于TDR,本发明对于变化程度较弱的局部缺陷的识别能力和多处缺陷的识别精度以及识别灵敏度更高,同时其对近端缺陷的识别能力也更强。3. Compared with TDR, the present invention has higher identification ability for local defects with weaker changes, identification accuracy and identification sensitivity for multiple defects, and its identification ability for near-end defects is also stronger.

4.本发明由于采取了通过对距离诊断图谱加距离窗处理的方法使畸变点更易表现出来,大大提高了定位精度。4. The present invention adopts the method of adding a distance window to the distance diagnostic atlas to make the distortion points easier to display, which greatly improves the positioning accuracy.

5.本发明采取了通过待测电缆与参考电缆距离诊断图谱的对比与选通门技术,找出相同位置处的畸变点并进行消除,以此消除电缆中间接头对电缆局部缺陷位置判断的影响。5. The present invention adopts the comparison of the distance diagnostic atlas between the cable to be tested and the reference cable and the gating gate technology to find out the distortion point at the same position and eliminate it, so as to eliminate the influence of the cable intermediate joint on the judgment of the local defect position of the cable .

6.本发明通过电缆的波速计算对电缆局部缺陷严重程度进行初步评估,在此基础上结合选通后反射系数谱模值拟合曲线对局部缺陷严重程度进行了进一步评估,能准确地评估电缆局部缺陷的严重程度。6. The present invention preliminarily evaluates the severity of local defects of the cable by calculating the wave velocity of the cable. On this basis, it further evaluates the severity of the local defects in combination with the analog value fitting curve of the reflection coefficient spectrum after gating, and can accurately evaluate the severity of the cable. Severity of local defects.

7.本发明的电缆缺陷诊断方法不受限于待测电缆的电压等级,传统的电缆缺陷诊断方法需要根据不同的电压等级选择不同的测试设备。7. The cable defect diagnosis method of the present invention is not limited to the voltage level of the cable to be tested. The traditional cable defect diagnosis method needs to select different test equipment according to different voltage levels.

附图说明Description of drawings

图1为本发明的电力电缆缺陷诊断方法的流程示意图。Fig. 1 is a schematic flow chart of the power cable defect diagnosis method of the present invention.

图2为本发明实施例1中绘制的被测电力电缆和参考电力电缆的对比距离诊断图谱,其中实线表示被测电力电缆的距离诊断图谱,虚线表示参考电力电缆的距离诊断图谱。Fig. 2 is the comparison distance diagnostic atlas of the measured power cable and the reference power cable drawn in Example 1 of the present invention, wherein the solid line represents the distance diagnostic atlas of the tested power cable, and the dotted line represents the distance diagnostic atlas of the reference power cable.

图3为本发明实施例1中绘制的经过选通门技术后的反射系数幅值谱对比图。其中虚线表示使用选通门技术后被测电力电缆的反射系数幅值谱,实线表示根据反射系数谱模值数学模型拟合得到的曲线。FIG. 3 is a comparison diagram of the reflection coefficient amplitude spectrum drawn in Embodiment 1 of the present invention after passing through the gate technology. The dotted line represents the reflection coefficient amplitude spectrum of the power cable under test after using the gate technology, and the solid line represents the curve fitted according to the mathematical model of the reflection coefficient spectrum modulus.

图4为本发明实施例2中绘制的局部缺陷距离诊断图谱。Fig. 4 is a diagnostic map of local defect distance drawn in Example 2 of the present invention.

具体实施方式Detailed ways

下面通过实施例对本发明进行具体的描述。有必要在此指出的是本实施例只用于对本发明进行进一步说明,不能理解为对本发明保护范围的限制。该领域的技术熟练人员可以根据上述本发明的内容做出一些非本质的改进和调整。The present invention is specifically described below by way of examples. It is necessary to point out that this embodiment is only used to further illustrate the present invention, and should not be construed as limiting the protection scope of the present invention. Those skilled in the art can make some non-essential improvements and adjustments based on the content of the present invention above.

实施例1Example 1

本实施例的电力电缆局部缺陷诊断方法的流程如图1所示,被测电力电缆和参考电力电缆的对比距离诊断图谱如图2所示,是针对100m ZR-YJV22-8.7/15电力电缆的局部缺陷诊断,缺陷类型为铜屏蔽层松动缺陷。诊断方法包括以下步骤:The flow chart of the method for diagnosing local defects in power cables of this embodiment is shown in Figure 1, and the comparison distance diagnostic map of the tested power cable and the reference power cable is shown in Figure 2, which is for the 100m ZR-YJV22-8.7/15 power cable Local defect diagnosis, the defect type is loose copper shielding layer defect. The diagnostic method includes the following steps:

(1)待测电缆数据测量(1) Data measurement of the cable to be tested

向被测100m ZR-YJV22-8.7/15电力电缆发射低压伪随机信号Vi,测量从电缆末端反射回来的反射信号Vr,通过求出电缆的反射系数谱的幅值|Γd(f)|以及反射系数谱的实部Real(Γd(f))和反射系数谱的虚部Imag(Γd(f))。Transmit a low-voltage pseudo-random signal V i to the 100m ZR-YJV22-8.7/15 power cable under test, measure the reflected signal V r reflected from the end of the cable, and pass Calculate the amplitude |Γ d (f)| of the reflection coefficient spectrum of the cable, the real part Real(Γ d (f)) of the reflection coefficient spectrum and the imaginary part Imag(Γ d (f)) of the reflection coefficient spectrum.

(2)待测电缆数据处理(2) Data processing of the cable to be tested

利用转换函数f→t′,将被测频域信号转换为t′域信号,然后对转换得到的Real(Γd(t′))进行快速傅里叶(FFT)变换,记录下能量最大的频率点f0′;然后对转换得到的Real(Γd(t′))与kaiser(凯瑟)窗相乘并进行快速傅里叶(FFT)变换得到初步处理数据KΓd,kaiser窗中的β取值为6;Using the conversion function f→t′, the measured frequency domain signal is converted into a t′ domain signal, and then the converted Real(Γ d (t′)) is subjected to fast Fourier (FFT) transformation, and the maximum energy is recorded frequency point f 0 ′; then multiply the converted Real(Γ d (t′)) with the Kaiser (Kaiser) window and perform fast Fourier (FFT) transformation to obtain the preliminary processing data KΓ d , the kaiser window The value of β is 6;

对KΓd做0赫兹至频率点f0′的DFT变换,将变换结果映射到原始距离诊断图谱D0中,其中0赫兹处映射距离为0米,f0′处映射距离为电缆长度100米。Do the DFT transformation from 0 Hz to the frequency point f 0 ′ on KΓ d , and map the transformation result to the original distance diagnostic map D 0 , where the mapping distance at 0 Hz is 0 meters, and the mapping distance at f 0 ′ is the cable length of 100 meters .

将得到的原始距离诊断图谱进行加距离窗长度s为5米的加窗处理,处理方式为:The obtained original distance diagnostic map is subjected to windowing processing with a distance window length s of 5 meters, and the processing method is as follows:

(3)参考电缆数据测量及处理(3) Reference cable data measurement and processing

将三相系统中的非被测相电缆作为参考电缆,然后利用步骤(1)相同方式求出参考电力电缆的反射系数谱的幅值|Γd1(f)|和反射系数谱的实部Real(Γd1(f))以及反射系数谱的虚部Imag(Γd1(f)),并进行步骤(2)中相同条件下的处理,得到处理后的距离诊断图谱E。Use the non-measured phase cable in the three-phase system as the reference cable, and then use the same method as step (1) to obtain the amplitude |Γ d1 (f)| of the reflection coefficient spectrum of the reference power cable and the real part of the reflection coefficient spectrum Real (Γ d1 (f)) and the imaginary part Imag(Γ d1 (f)) of the reflection coefficient spectrum, and perform the processing under the same conditions in step (2), to obtain the processed distance diagnostic map E.

(4)电力电缆局部缺陷位置确定(4) Determination of the location of local defects in power cables

对比距离诊断图谱D和距离诊断图谱E,如图2所示,利用选通门技术消除距离诊断图谱D中与距离诊断图谱E相同位置处的畸变点,得到局部缺陷距离诊断图谱F。从图2可以发现在70米的位置存在一个明显的畸变点,该处正是设置的局部缺陷点。Comparing the distance diagnostic map D and the distance diagnostic map E, as shown in Figure 2, using the gate technology to eliminate the distortion points at the same position as the distance diagnostic map E in the distance diagnostic map D, and obtain the local defect distance diagnostic map F. From Figure 2, it can be found that there is an obvious distortion point at the position of 70 meters, which is exactly the set local defect point.

(5)电缆局部缺陷严重程度评估(5) Severity assessment of cable local defects

对得到的局部缺陷距离诊断图谱进行快速傅里叶反变换(IFFT),得到变换后的反射系数谱t′域曲线,并利用转换函数t′→f转换为Real(Γd2(f))。找到Real(Γd2(f))中每个极大值点对应的频率fk,利用公式求出被测电力电缆的平均波速vc=1.7247×108米/秒,测得新电缆波速v0=1.7261×108米/秒。其中N为Real(Γd2)或Imag(Γd2)中极大值点或极小值点的个数。vc与v0两者相差0.81%<1%,说明被测电缆局部缺陷较轻。The inverse fast Fourier transform (IFFT) is performed on the obtained local defect distance diagnosis map to obtain the transformed reflection coefficient spectrum t′ domain curve, which is transformed into Real(Γ d2 (f)) using the conversion function t′→f. Find the frequency f k corresponding to each maximum point in Real(Γ d2 (f)), using the formula Calculate the average wave velocity v c of the tested power cable = 1.7247×10 8 m/s, and measure the wave velocity v 0 of the new cable = 1.7261×10 8 m/s. Where N is the number of maximum or minimum points in Real(Γ d2 ) or Imag(Γ d2 ). The difference between v c and v 0 is 0.81%<1%, indicating that the local defect of the tested cable is relatively light.

为了进一步评估被测电缆局部缺陷的严重程度,建立电缆反射系数谱模值数学模型:In order to further evaluate the severity of the local defects of the tested cable, a mathematical model of the spectral modulus of the cable reflection coefficient is established:

abs(Γd2(f))=a·eb·f+c·ed·f abs(Γ d2 (f))=a·e b·f +c·e d·f

利用建立的数学模型对被测电缆测量得到的反射系数谱采用选通门技术后的模值|Γd2(f)|进行数据拟合,拟合结果为如图3所示,求出较高频率极值点fk处对应的拟合值并由公式Use the established mathematical model to perform data fitting on the reflection coefficient spectrum measured by the measured cable using the gate technology |Γ d2 (f)|, and the fitting result is As shown in Figure 3, the fitting value corresponding to the extreme point f k of the higher frequency is obtained and calculated by the formula

error=std((|Γd2(fk)|-abs(Γd2(fk)))/abs(Γd2(fk)))×100%error=std((|Γ d2 (f k )|-abs(Γ d2 (f k )))/abs(Γ d2 (f k )))×100%

求出|Γd2(f)|与拟合曲线的相对差值的标准差error=1.16%<5%,说明被测电力电缆的局部缺陷较轻,印证了此时被测电力电缆存在铜屏蔽层松动的缺陷。Calculate the standard deviation of the relative difference between |Γ d2 (f)| and the fitting curve error=1.16%<5%, indicating that the local defect of the tested power cable is relatively light, which confirms that the tested power cable has copper shielding at this time Defects of loose layers.

实施例2Example 2

本实施例的电力电缆局部缺陷诊断方法的流程如图1所示,被测电力电缆和参考电力电缆的对比距离诊断图谱如图4所示,针对1500m 10kV XLPE电力电缆进行局部缺陷诊断,缺陷类型也绝缘介质严重变形缺陷,包括以下步骤:The process flow of the power cable local defect diagnosis method of this embodiment is shown in Figure 1, and the comparison distance diagnosis map of the tested power cable and the reference power cable is shown in Figure 4, for the local defect diagnosis of 1500m 10kV XLPE power cable, the defect type Also severe deformation defects of the insulating medium, including the following steps:

(1)待测电缆数据测量(1) Data measurement of the cable to be tested

向被测1500m ZR-YJV22-8.7/15电力电缆发射低压高频窄脉冲Vi,测量从电缆末端反射回来的反射信号Vr,通过求出电缆的反射系数谱的幅值|Γd(f)|以及反射系数谱的实部Real(Γd(f))和反射系数谱的虚部Imag(Γd(f))。Transmit low-voltage high-frequency narrow pulse V i to the 1500m ZR-YJV22-8.7/15 power cable under test, measure the reflected signal V r reflected from the end of the cable, and pass Calculate the amplitude |Γ d (f)| of the reflection coefficient spectrum of the cable, the real part Real(Γ d (f)) of the reflection coefficient spectrum and the imaginary part Imag(Γ d (f)) of the reflection coefficient spectrum.

(2)待测电缆数据处理(2) Data processing of the cable to be tested

利用转换函数f→t′,将被测频域信号转换为t′域信号,然后对转换得到的Imag(Γd(t′))进行离散傅里叶(DFT)变换,记录下能量最大的频率点f0′;然后对转换得到的Imag(Γd(t′))与kaiser(凯瑟)窗相乘并进行离散傅里叶(DFT)变换到初步处理数据KΓd,kaiser窗中的β取值为8;Using the conversion function f→t′, the measured frequency domain signal is converted into a t′ domain signal, and then the converted Imag(Γ d (t′)) is subjected to discrete Fourier (DFT) transformation, and the maximum energy frequency point f 0 ′; then the transformed Imag(Γ d (t′)) is multiplied by the kaiser (Kaiser) window, and the discrete Fourier (DFT) transform is carried out to the preliminary processing data KΓ d , the kaiser window The value of β is 8;

对KΓd做0赫兹至频率点f0′的DFT变换,将变换结果映射到原始距离诊断图谱D0中,其中0Hz处映射距离为0米,f0′处映射距离为电缆长度1500米。Perform DFT transformation from 0 Hz to frequency point f 0 ′ on KΓ d , and map the transformation result to the original distance diagnostic map D 0 , where the mapping distance at 0 Hz is 0 meters, and the mapping distance at f 0 ′ is the cable length of 1500 meters.

将得到的原始距离诊断图谱进行加距离窗长度s为30米的加窗处理,处理方式为:The obtained original distance diagnostic map is subjected to windowing processing with a distance window length s of 30 meters, and the processing method is as follows:

(3)参考电缆数据测量及处理(3) Reference cable data measurement and processing

将三相系统中的非待测相电缆作为参考电缆,然后利用步骤(1)相同方式求出参考电力电缆的反射系数谱的幅值|Γd1(f)|以及反射系数谱的实部Real(Γd1(f))和反射系数谱的虚部Imag(Γd1(f)),并进行步骤(2)中相同条件下的处理,得到处理后的距离诊断图谱E。Use the non-tested phase cable in the three-phase system as the reference cable, and then use the same method as step (1) to obtain the amplitude |Γ d1 (f)| of the reflection coefficient spectrum of the reference power cable and the real part of the reflection coefficient spectrum Real (Γ d1 (f)) and the imaginary part Imag(Γ d1 (f)) of the reflection coefficient spectrum, and perform the processing under the same conditions in step (2), to obtain the processed distance diagnostic map E.

(4)电力电缆局部缺陷位置确定(4) Determination of the location of local defects in power cables

对比距离诊断图谱D和距离诊断图谱E,利用选通门技术消除距离诊断图谱D中与距离诊断图谱E相同位置处的畸变点,得到局部缺陷距离诊断图谱F,如图3所示。从图3可以发现在500米和1200米处存在明显的畸变点,该处正是设置的局部缺陷点。Compare the distance diagnostic atlas D and distance diagnostic atlas E, and use the gate technology to eliminate the distortion points at the same position in the distance diagnostic atlas D and distance diagnostic atlas E, and obtain the local defect distance diagnostic atlas F, as shown in Figure 3. From Figure 3, it can be found that there are obvious distortion points at 500 meters and 1200 meters, which are exactly the set local defect points.

(4)电缆局部缺陷严重程度评估(4) Severity assessment of cable local defects

对得到的局部缺陷距离诊断图谱进行离散傅里叶反变换(IDFT),得到变换后的反射系数谱t′域曲线,并利用转换函数t′→f转换为Imag(Γd2(f))。找到Imag(Γd2(f))中每个极小值点对应的频率fk,利用公式求出被测电力电缆的平均波速v0=1.7217×108米/秒,测得新电缆波速v0=1.7261×108米/秒。其中N为Imag(Γd2)中极大值点或极小值点的个数。vc与v0两者相差2.55%>1%,说明被测电缆局部缺陷比较严重。Inverse discrete Fourier transform (IDFT) is performed on the obtained local defect distance diagnostic map to obtain the transformed reflection coefficient spectrum t′ domain curve, which is transformed into Imag(Γ d2 (f)) using the transfer function t′→f. Find the frequency f k corresponding to each minimum point in Imag(Γ d2 (f)), use the formula Calculate the average wave velocity v 0 of the tested power cable = 1.7217×10 8 m/s, and measure the new cable wave velocity v 0 = 1.7261×10 8 m/s. Where N is the number of maximum or minimum points in Imag(Γ d2 ). The difference between v c and v 0 is 2.55%>1%, indicating that the local defects of the tested cable are relatively serious.

为了进一步评估被测电缆局部缺陷的严重程度,建立电缆反射系数谱模值数学模型:In order to further evaluate the severity of the local defects of the tested cable, a mathematical model of the spectral modulus of the cable reflection coefficient is established:

abs(Γd2(f))=a·eb·f+c·ed·f abs(Γ d2 (f))=a·e b·f +c·e d·f

利用建立的数学模型对被测电缆测量得到的反射系数谱采用选通门技术后的模值|Γd2(f)|进行数据拟合,拟合结果为求出较高频率极值点fk处对应的拟合值并由公式Use the established mathematical model to perform data fitting on the reflection coefficient spectrum measured by the measured cable using the gate technology |Γ d2 (f)|, and the fitting result is Calculate the fitting value corresponding to the extreme point f k of the higher frequency and use the formula

error=std((|Γd2(fk)|-abs(Γd2(fk)))/abs(Γd2(fk)))×100%error=std((|Γ d2 (f k )|-abs(Γ d2 (f k )))/abs(Γ d2 (f k )))×100%

求出|Γd2(f)|与拟合曲线的相对差值的标准差error=16.14%>10%,说明被测电力电缆的局部缺陷比较严重,印证了此时被测电力电缆存在绝缘介质严重变形的严重缺陷。Calculate the standard deviation of the relative difference between |Γ d2 (f)| and the fitting curve error=16.14%>10%, indicating that the local defects of the tested power cable are relatively serious, which confirms that the tested power cable has an insulating medium at this time Severely deformed serious fault.

Claims (9)

1.一种高灵敏度电力电缆局部缺陷诊断方法,其特征在于:包括以下步骤:1. A high-sensitivity power cable local defect diagnosis method, is characterized in that: comprise the following steps: (1)待测电缆数据测量(1) Data measurement of the cable to be tested 向被测电力电缆发射低压线性调频、伪随机或者高频窄脉冲的信号Vi,测量从电缆末端反射回来的反射信号Vr,通过求出电缆的反射系数谱的幅值|Γd(f)|以及反射系数谱的实部Real(Γd(f))和反射系数谱的虚部Imag(Γd(f)),其中f为信号频率;Transmit a low-voltage linear frequency modulation, pseudo-random or high-frequency narrow pulse signal V i to the power cable under test, measure the reflected signal V r reflected from the end of the cable, and pass Find the amplitude |Γ d (f)| of the reflection coefficient spectrum of the cable and the real part Real(Γ d (f)) of the reflection coefficient spectrum and the imaginary part Imag(Γ d (f)) of the reflection coefficient spectrum, where f is the signal frequency; (2)待测电缆数据处理(2) Data processing of the cable to be tested 利用转换函数f→t′,将被测频域信号f转换为t′域信号,然后对转换得到的Real(Γd(t′))或Imag(Γd(t′))进行快速傅里叶变换或者离散傅里叶变换,记录下能量最大的频率点f0′;然后对转换得到的Real(Γd(t′))或Imag(Γd(t′))与kaiser窗函数相乘并进行快速傅里叶变换或者离散傅里叶变换,得到初步处理数据KΓdUsing the conversion function f→t′, the measured frequency domain signal f is converted into a t′ domain signal, and then the converted Real(Γ d (t′)) or Imag(Γ d (t′)) is fast Fourier leaf transform or discrete Fourier transform, record the frequency point f 0 ′ with the highest energy; then multiply the converted Real(Γ d (t′)) or Imag(Γ d (t′)) with the Kaiser window function And perform Fast Fourier Transform or Discrete Fourier Transform to obtain preliminary processing data KΓd ; 对得到的初步处理数据KΓd做0赫兹至频率点f0′的离散傅里叶变换,将变换结果映射到原始距离诊断图谱D0中,对原始距离诊断图谱D0进行加距离窗处理,得到距离诊断图谱D,其中0赫兹处映射距离为0米,频率点f0′处映射距离为电力电缆长度l;Do the discrete Fourier transform from 0 Hz to the frequency point f 0 ′ on the obtained preliminary processing data KΓ d , map the transformation result to the original distance diagnostic map D 0 , and add a distance window to the original distance diagnostic map D 0 , Obtain the distance diagnostic map D, wherein the mapping distance at 0 Hz is 0 meters, and the mapping distance at the frequency point f 0 ′ is the length l of the power cable; (3)参考电缆数据测量及处理(3) Reference cable data measurement and processing 将三相系统中的非被测相电力电缆作为参考电力电缆,然后利用步骤(1)相同方式求出参考电力电缆的反射系数谱的幅值|Γd1(f)|以及反射系数谱的实部Real(Γd1(f))和反射系数谱的虚部Imag(Γd1(f)),并进行步骤(2)中相同方式的处理,得到处理后的距离诊断图谱E;Use the non-measured phase power cable in the three-phase system as the reference power cable, and then use the same method as step (1) to obtain the amplitude |Γ d1 (f)| of the reflection coefficient spectrum of the reference power cable and the real value of the reflection coefficient spectrum Part Real (Γ d1 (f)) and the imaginary part Imag (Γ d1 (f)) of the reflection coefficient spectrum, and carry out the processing in the same way in the step (2), obtain the distance diagnostic map E after processing; (4)电力电缆局部缺陷位置确定(4) Determination of the location of local defects in power cables 对比距离诊断图谱D和处理后的距离诊断图谱E,利用选通门技术消除距离诊断图谱D中与处理后的距离诊断图谱E相同位置处的畸变点,得到局部缺陷距离诊断图谱F,从局部缺陷距离诊断图谱F中找到的畸变点,即为电力电缆局部缺陷位置;Comparing the distance diagnostic map D and the processed distance diagnostic map E, using the gate technology to eliminate the distortion points at the same position in the distance diagnostic map D and the processed distance diagnostic map E, to obtain the local defect distance diagnostic map F, from the local The distortion point found in the defect distance diagnostic map F is the local defect position of the power cable; (5)电力电缆局部缺陷判断(5) Judgment of local defects of power cables 对得到的局部缺陷距离诊断图谱进行离散傅里叶反变换或快速傅里叶反变换,得到变换后的t′域反射系数谱曲线,并利用转换函数t′→f将t′域反射系数谱转换为Real(Γd2(f))或Imag(Γd2(f)),然后找到Real(Γd2(f))或Imag(Γd2(f))中每个极大值点或极小值点对应的频率fk,利用公式求出被测电力电缆的平均波速,并将vc与同规格的新电力电缆波速v0进行比较,若vc与v0相差1%及以上,说明被测电缆存在局部缺陷,其中N为Real(Γd2)或Imag(Γd2)中极大值点或极小值点的个数。Inverse discrete Fourier transform or inverse fast Fourier transform is performed on the obtained local defect distance diagnostic map to obtain the transformed t′-domain reflection coefficient spectrum curve, and use the conversion function t′→f to convert the t′-domain reflection coefficient spectrum Convert to Real(Γ d2 (f)) or Imag(Γ d2 (f)), and then find each maximum point or minimum value in Real(Γ d2 (f)) or Imag(Γ d2 (f)) The frequency f k corresponding to the point, using the formula Find the average wave velocity of the power cable under test, and compare v c with the wave velocity v 0 of a new power cable of the same specification. If the difference between v c and v 0 is 1% or more, it means that there is a local defect in the test cable, where N is The number of maximum or minimum points in Real(Γ d2 ) or Imag(Γ d2 ). 2.根据权利要求1所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于,通过下述方法进一步评估被测电力电缆局部缺陷的严重程度:2. The method for diagnosing local defects of a high-sensitivity power cable according to claim 1, wherein the severity of the local defect of the tested power cable is further evaluated by the following method: 建立电缆反射系数谱模值数学模型Establishment of Mathematical Model of Spectrum Modulus of Cable Reflection Coefficient abs(Γd2(f))=a·eb·f+c·ed·f abs(Γ d2 (f))=a·e b·f +c·e d·f 利用建立的数学模型对被测电力电缆测量得到的反射系数谱采用选通门技术后的模值|Γd2(f)|进行数据拟合,求较高频率极值点fk处对应的拟合值,并由下面公式计算得到缺陷程度error进行评估:Use the established mathematical model to perform data fitting on the reflection coefficient spectrum measured by the measured power cable using the gate technology |Γ d2 (f)|, and find the corresponding quasi-parameter at the higher frequency extreme point f k Combined value, and the defect degree error calculated by the following formula for evaluation: error=std((|Γd2(fk)|-abs(Γd2(fk)))/abs(Γd2(fk)))×100%error=std((|Γ d2 (f k )|-abs(Γ d2 (f k )))/abs(Γ d2 (f k )))×100% 当error<5%时,电力电缆局部缺陷较轻,当5%≤error≤10%时,电力电缆局部缺陷程度中等,当error>10%时,电力电缆局部缺陷非常严重,公式中std为标准差。When the error<5%, the local defect of the power cable is relatively light; when 5%≤error≤10%, the local defect of the power cable is moderate; when the error>10%, the local defect of the power cable is very serious, and std in the formula is the standard Difference. 3.根据权利要求1或2所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于,所述kaiser窗函数中的β取值满足:3. according to claim 1 and 2 described high-sensitivity power cable local defect diagnosis methods, it is characterized in that, the β value in the described kaiser window function satisfies: 其中α为旁瓣衰减倍数。Where α is the side lobe attenuation multiple. 4.根据权利要求1或2所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于,原始距离诊断图谱D0采用下述公式进行加距离窗处理:4. according to claim 1 and 2 described high-sensitivity power cable local defect diagnostic method, it is characterized in that, original distance diagnostic atlas D 0 adopts following formula to carry out adding distance window processing: 其中s为窗口长度,取值不大于距离诊断图谱D0中的空间分辨率,D为处理后得到的距离诊断图谱。Where s is the window length, and the value is not greater than the spatial resolution in the distance diagnostic atlas D 0 , and D is the distance diagnostic atlas obtained after processing. 5.根据权利要求3所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于,原始距离诊断图谱D0采用下述公式进行加距离窗处理:5. the high-sensitivity power cable local defect diagnosis method according to claim 3, is characterized in that, original distance diagnosis atlas D 0 adopts following formula to carry out adding distance window processing: 其中s为窗口长度,取值不大于距离诊断图谱D0中的空间分辨率,D为处理后得到的距离诊断图谱。Where s is the window length, and the value is not greater than the spatial resolution in the distance diagnostic atlas D 0 , and D is the distance diagnostic atlas obtained after processing. 6.根据权利要求1或2所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于:步骤(5)中同规格的新电缆波速v0由公式计算获得,其中L和C分别为同规格的新电缆单位长度的电感和电容,或者采用时域反射法测取。6. The method for diagnosing local defects of high-sensitivity power cables according to claim 1 or 2, characterized in that: in step (5), the new cable wave velocity v of the same specification is given by the formula Obtained by calculation, where L and C are the inductance and capacitance per unit length of a new cable of the same specification, or measured by time domain reflection method. 7.根据权利要求3所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于:步骤(5)中同规格的新电缆波速v0由公式计算获得,其中L和C分别为同规格的新电缆单位长度的电感和电容,或者采用时域反射法测取。7. The high-sensitivity power cable local defect diagnosis method according to claim 3 is characterized in that: in the step (5), the new cable wave velocity v of the same specification is given by the formula Obtained by calculation, where L and C are the inductance and capacitance per unit length of a new cable of the same specification, or measured by time domain reflection method. 8.根据权利要求4所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于:步骤(5)中同规格的新电缆波速v0由公式计算获得,其中L和C分别为同规格的新电缆单位长度的电感和电容,或者采用时域反射法测取。8. The high-sensitivity power cable local defect diagnosis method according to claim 4 is characterized in that: in step (5), the new cable wave velocity v of the same specification is given by the formula Obtained by calculation, where L and C are the inductance and capacitance per unit length of a new cable of the same specification, or measured by time domain reflection method. 9.根据权利要求5所述的高灵敏度电力电缆局部缺陷诊断方法,其特征在于:步骤(5)中同规格的新电缆波速v0由公式计算获得,其中L和C分别为同规格的新电缆单位长度的电感和电容,或者采用时域反射法测取。9. The high-sensitivity power cable local defect diagnosis method according to claim 5 is characterized in that: in the step (5), the new cable wave velocity v of the same specification is given by the formula Obtained by calculation, where L and C are the inductance and capacitance per unit length of a new cable of the same specification, or measured by time domain reflection method.
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