CN106405326A - Time-domain fault range finding method for co-tower double-loop DC power transmission line based on single-loop electrical quantity - Google Patents
Time-domain fault range finding method for co-tower double-loop DC power transmission line based on single-loop electrical quantity Download PDFInfo
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Abstract
本发明公开了一种基于单回电气量同塔双回直流输电线路时域故障测距方法,包括以下步骤:1、提取阻抗矩阵和导纳矩阵;2、得到电压解耦矩阵和电流解耦矩阵;3、根据得到的电压解耦矩阵构造消去地模分量的单回电压相模变换矩阵,得到消去地模分量的单回电压差模分量;4、根据得到的电流解耦矩阵构造消去地模分量的单回电流相模变换矩阵,得到消去地模分量的单回电流差模分量;5、根据不同极线故障时各个模量的分布特点选取最为突出的分量,选择该模量对应的模量参数;6、沿线电压分布计算;7、构造基于混合模量的故障定位判据;8、计算故障时刻;9、选取冗余数据窗。具有计算精度高、可靠性强、所需数据时间窗短和易于实现等优点。
The invention discloses a time-domain fault location method for double-circuit direct current transmission lines on the same tower based on single-circuit electrical quantity, comprising the following steps: 1. Extracting impedance matrix and admittance matrix; 2. Obtaining voltage decoupling matrix and current decoupling 3. According to the obtained voltage decoupling matrix, construct the phase-mode transformation matrix of the single-circuit voltage that eliminates the ground-mode component, and obtain the single-circuit voltage differential-mode component that eliminates the ground-mode component; 4. According to the obtained current decoupling matrix, construct the eliminated ground-mode The single-circuit current phase-mode transformation matrix of the component is obtained to eliminate the single-circuit current differential mode component of the ground mode component; 5. According to the distribution characteristics of each modulus when different polar lines are faulted, select the most prominent component, and select the corresponding modulus Parameters; 6. Calculation of voltage distribution along the line; 7. Construction of fault location criteria based on mixed modulus; 8. Calculation of fault time; 9. Selection of redundant data windows. It has the advantages of high calculation accuracy, strong reliability, short required data time window and easy implementation.
Description
技术领域technical field
本发明涉及电力系统继电保护技术领域,具体涉及一种基于单回电气量同塔双回直流输电线路时域故障测距方法,该时域故障测距算法是一种基于同塔双回直流线路的单回测量数据的双端时域测距算法。The invention relates to the technical field of power system relay protection, in particular to a time-domain fault location method for double-circuit DC transmission lines on the same tower based on single-circuit electrical quantity. A dual-terminal time-domain ranging algorithm for single-return measurement data of a line.
背景技术Background technique
高压直流输电具有输送容量大,控制灵活迅速,不存在同步稳定问题等优势,在远距离大容量电能传输,异步电网互联领域有着广泛的应用。随着社会经济的发展,电网建设成本因为土地资源日益紧张而逐渐增加。高压线路同杆架设能有效利用输电走廊,不仅在交流电网中应用广泛,近年来在直流工程中也开始得到具体应用。High-voltage direct current transmission has the advantages of large transmission capacity, flexible and rapid control, and no synchronization and stability problems. It has a wide range of applications in the field of long-distance large-capacity power transmission and asynchronous grid interconnection. With the development of society and economy, the cost of power grid construction is gradually increasing due to the increasingly tight land resources. The erection of high-voltage lines on the same pole can effectively utilize the transmission corridor. It is not only widely used in AC power grids, but also has begun to be specifically applied in DC projects in recent years.
高压直流输电线路送电距离一般超过1000km,容易遭受故障。在故障发生后,实现快速准确的故障定位能减少巡线工作量,快速恢复供电,以保证交直流互联电网的安全稳定运行。在高压直流线路故障测距方法中,基于分布参数的时域测距方法由于具有不依赖于初始行波波头的准确捕捉以及行波达到时刻的准确标定,对采样装置要求低的优点,能够作为现有行波测距方法的有效补充。The transmission distance of HVDC transmission lines generally exceeds 1000km and is prone to failure. After a fault occurs, fast and accurate fault location can reduce the workload of line inspection and quickly restore power supply to ensure the safe and stable operation of the AC-DC interconnected grid. Among the fault location methods of HVDC lines, the time-domain location method based on distribution parameters has the advantages of not relying on the accurate capture of the initial traveling wave head and the accurate calibration of the arrival time of the traveling wave, and has the advantages of low requirements on the sampling device. There is an effective complement to the traveling wave ranging method.
然而,目前直流线路故障测距方法大多局限于单回双极直流线路,在方法中只需考虑结构对称的双极线之间的电磁耦合影响。但是对于同塔双回直流输电线路,由于双回线路四条极线间均存在相互作用的电磁耦合关系,且实际工程中同塔双回直流线路不采用换位措施,造成其故障耦合特性非常复杂。更值得引起注意的是,在实际应用中由于各回直流系统的控制保护仍然是基于本回线路电气量信息,必然无法实现各耦合电气量的完全解耦,这些因素均大大增加了同塔双回直流输电线路故障分析及其准确故障定位的难度。However, most current DC line fault location methods are limited to single-circuit bipolar DC lines, and only need to consider the influence of electromagnetic coupling between structurally symmetrical bipolar lines in the method. However, for the double-circuit DC transmission line on the same tower, due to the electromagnetic coupling relationship between the four poles of the double-circuit line, and the double-circuit DC line on the same tower does not use transposition measures in actual engineering, its fault coupling characteristics are very complicated . What is more noteworthy is that in practical applications, since the control and protection of each DC system is still based on the electrical quantity information of the current circuit, it is inevitable that the complete decoupling of each coupled electrical quantity cannot be achieved. Fault analysis of DC transmission lines and the difficulty of accurate fault location.
因此,现有的单回直流输电线路的相模变换方法以及故障定位算法不再适用同塔双回直流线路,亟需针对同塔双回直流输电线路的特点,研究其适用的故障测距方法。Therefore, the existing phase-mode conversion methods and fault location algorithms for single-circuit DC transmission lines are no longer applicable to double-circuit DC lines on the same tower. It is urgent to study the applicable fault location method according to the characteristics of double-circuit DC transmission lines on the same tower.
发明内容Contents of the invention
本发明的目的在于提出一种基于单回电气量同塔双回直流输电线路时域故障测距方法,该时域故障测距方法考虑到实际工程中同塔双回直流输电线路不采用对称换位措施,且各回直流系统的控制保护仍然基于本回电气量信息,构造了消去地模分量的差模分量。同时根据非故障点的线路两端沿线计算电压在故障时刻附近具有最大差值的特点,本发明定义了非故障点最大电压差值区段。所提故障测距算法所需数据窗短,故障测距精度高,不受过渡电阻和故障位置的影响。The purpose of the present invention is to propose a time-domain fault location method for double-circuit DC transmission lines on the same tower based on single-circuit electrical quantities. Position measures, and the control and protection of each return DC system is still based on the electrical quantity information of this return, and the differential mode component that eliminates the ground mode component is constructed. At the same time, according to the feature that the calculated voltage along the two ends of the line at the non-fault point has the largest difference near the fault time, the present invention defines the maximum voltage difference section at the non-fault point. The proposed fault location algorithm requires a short data window, high fault location accuracy, and is not affected by transition resistance and fault location.
本发明的目的通过下述技术方案实现:一种基于单回电气量同塔双回直流输电线路时域故障测距方法,包括以下步骤:The purpose of the present invention is achieved through the following technical solutions: a time-domain fault location method for double-circuit DC transmission lines on the same tower based on single-circuit electrical quantity, comprising the following steps:
(1)提取输电线路的阻抗矩阵和导纳矩阵:同塔双回输电线路不可视为对称线路,需要根据实际的阻抗矩阵[Zphase]和导纳矩阵[Yphase]构造相模变换矩阵。(1) Extract the impedance matrix and admittance matrix of the transmission line: the double-circuit transmission line on the same tower cannot be regarded as a symmetrical line, and the phase-to-mode transformation matrix needs to be constructed according to the actual impedance matrix [Z phase ] and admittance matrix [Y phase ].
(2)构造同塔双回直流输电线路解耦矩阵:分别用1P、1N和2P、2N分别代表同塔架设的I回正极、负极和II回正极、负极线路。根据电力系统电磁暂态理论可以得到同塔双回的均匀传输线方程:(2) Construct the decoupling matrix of double-circuit DC transmission lines on the same tower: 1P, 1N and 2P, 2N respectively represent the positive and negative poles of the I circuit and the positive and negative poles of the II circuit erected on the same tower. According to the electromagnetic transient theory of the power system, the equation of the uniform transmission line with double circuits on the same tower can be obtained:
式中,[Uphase]=[u1P u1N u2p u2N]T为极线电压列向量;[Iphase]=[i1P i1N i2p i2N]T为极线电流列向量。In the formula, [U phase ]=[u 1P u 1N u 2p u 2N ] T is the polar line voltage column vector; [I phase ]=[i 1P i 1N i 2p i 2N ] T is the polar line current column vector.
将上式整理可得二阶微分方程:Arrange the above formula to get the second order differential equation:
根据矩阵特征值理论,将把两个矩阵对角化,可知[Zphase][Yphase]的特征值矩阵为[Λ],特征向量矩阵[Tv],因此存在下式:According to the matrix eigenvalue theory, the two matrices will be diagonalized. It can be seen that the eigenvalue matrix of [Z phase ][Y phase ] is [Λ], and the eigenvector matrix [T v ], so there is the following formula:
[Zphase][Yphase]=[Tv][Λ][Tv]-1,[Z phase ][Y phase ]=[T v ][Λ][T v ] -1 ,
考虑到[Zphase][Yphase]=[[Yphase][Zphase]]T,则存在以下关系式:Considering [Z phase ][Y phase ]=[[Y phase ][Z phase ]] T , the following relationship exists:
[Tv]-1=[Ti]T,[T v ] -1 = [T i ] T ,
以上就得到了电压解耦矩阵[Tv]、电流解耦矩阵[Ti]。在此设[Tv]=[Tvab]4×4、[Ti]=[Tiab]4×4,a,b=1,2,3,4,其中Tvab和Tiab均是与频率有关的数值,仅当线路采用对称换位时为固定常数。The voltage decoupling matrix [T v ] and the current decoupling matrix [T i ] are obtained above. Let [T v ]=[T vab ] 4×4 , [T i ]=[T iab ] 4×4 , a,b=1,2,3,4, where T vab and T iab are the same as A frequency-dependent value that is a fixed constant only when the line uses symmetrical transposition.
(3)构造消去地模分量的单回电压相模变换矩阵:(3) Construct a single-circuit voltage phase-mode transformation matrix that eliminates the ground-mode component:
由于采用传统的单回相模变换解耦矩阵不能消去地模分量,由于地模分量受大地电导率和频率的影响较大,从而使得到的差模分量较不稳定,这对于实现准确故障定位是不利的。因此,有必要构造一个新的单回变换矩阵以消除地模分量的影响。根据以上得到的电压解耦矩阵[Tv],用各个模量线性表示线路各极电压量。求出同塔双回直流输电线路测量端的各模量电压瞬时值,其中0表示地模分量,1、2和3表示第一线模分量、第二线模分量和第三线模分量,则各极的电压量可以表示为:Since the traditional single-circuit phase-mode transformation decoupling matrix cannot eliminate the ground mode component, and because the ground mode component is greatly affected by the conductivity and frequency of the ground, the resulting differential mode component is relatively unstable, which is critical for accurate fault location. Adverse. Therefore, it is necessary to construct a new single-return transformation matrix to eliminate the influence of the ground model component. According to the voltage decoupling matrix [T v ] obtained above, each modulus is used to linearly represent the voltage of each pole of the line. Find the instantaneous value of each modulus voltage at the measuring end of the double-circuit DC transmission line on the same tower, where 0 represents the ground mode component, 1, 2 and 3 represent the first line mode component, the second line mode component and the third line mode component, then each pole The voltage quantity can be expressed as:
根据[Tv]中地模分量在单回I正极、负极和单回II正极、负极电压中所占比例构造单回变换矩阵。根据新的单回变换矩阵即可得到单回线路电压消除地模分量后的电压分量。According to the ratio of the ground mode component in [T v ] to the positive and negative voltages of the single circuit I and the positive and negative voltages of the single circuit II, the single-circuit transformation matrix is constructed. According to the new single-circuit transformation matrix, the voltage component of the single-circuit line voltage after eliminating the ground mode component can be obtained.
对于I回线路,新的单回变换矩阵形式为:For the I-circuit line, the new single-circuit transformation matrix form is:
式中:[Tv_I_eli0]是I线路的消去地模分量的电压变换矩阵;Udif_I_eli0是I回线路消去地模后得到的电压差模分量;Tv11、Tv21是1P、1N电压分量在[Tv]中地模分量的系数。In the formula: [T v_I_eli0 ] is the voltage transformation matrix of the ground mode component of the I circuit; U dif_I_eli0 is the voltage differential mode component of the I circuit line after the ground mode is eliminated; T v11 and T v21 are the 1P and 1N voltage components in [ T v ] in the coefficient of the earth mode component.
对于II回线路,新的单回变换矩阵形式为:For circuit II, the form of the new single-circuit transformation matrix is:
式中:[Tv_II_eli0]是II线路的消去地模分量的电压变换矩阵;Udif_II_eli0是II回线路消去地模后得到的电压差模分量;Tv31、Tv41是2P、2N电压分量在[Tv]中地模分量的系数。In the formula: [T v_II_eli0 ] is the voltage transformation matrix of the ground mode component of the II line; U dif_II_eli0 is the voltage differential mode component of the II circuit line after the ground mode is eliminated; T v31 and T v41 are the 2P and 2N voltage components in [ T v ] in the coefficient of the earth mode component.
(4)构造消去地模分量的单回电流相模变换矩阵:(4) Construct a single-circuit current phase-mode transformation matrix that eliminates the ground-mode component:
根据以上得到的电流解耦矩阵[Ti],用各个模量线性表示线路各极电流量。求出同塔双回直流输电线路测量端的各模量电流瞬时值,其中0表示地模分量,1、2和3表示第一线模分量、第二线模分量和第三线模分量,则各极的电压量可以表示为:According to the current decoupling matrix [T i ] obtained above, use each modulus to linearly represent the current of each pole of the line. Find the instantaneous value of each modulus current at the measuring end of the double-circuit DC transmission line on the same tower, where 0 represents the ground mode component, 1, 2 and 3 represent the first line mode component, the second line mode component and the third line mode component, then each pole The voltage quantity can be expressed as:
根据[Ti]中地模分量在单回I正极、负极和单回II正极、负极电流中所占比例构造单回变换矩阵。根据新的单回变换矩阵即可得到单回线路电流消除地模分量后的电流分量。According to the proportion of the ground mode component in [T i ] in the positive and negative poles of single-circuit I and the positive and negative poles of single-circuit II, the single-circuit transformation matrix is constructed. According to the new single-circuit transformation matrix, the current component of the single-circuit line current after eliminating the ground-mode component can be obtained.
对于I回线路,新的单回变换矩阵形式为:For the I-circuit line, the new single-circuit transformation matrix form is:
式中:[Ti_I_eli0]是I线路的消去地模分量的电流变换矩阵;Idif_I_eli0是I回线路消去地模后得到的电流差模分量;Ti11、Ti21是1P、1N电流分量在[Ti]中地模分量的系数。In the formula: [T i_I_eli0 ] is the current transformation matrix of the ground mode component of the I line; I dif_I_eli0 is the current differential mode component obtained after the ground mode is eliminated in the I circuit line; T i11 and T i21 are 1P and 1N current components in [ T i ] in the coefficient of the earth mode component.
对于II回线路,新的单回变换矩阵形式为:For circuit II, the form of the new single-circuit transformation matrix is:
式中:[Ti_II_eli0]是II线路的消去地模分量的电流变换矩阵;Idif_II_eli0是II回线路消去地模后得到的电流差模分量;Ti31、Ti41是2P、2N电流分量在[Ti]中地模分量的系数。In the formula: [T i_II_eli0 ] is the current transformation matrix of the ground mode component of the II line; I dif_II_eli0 is the current differential mode component obtained after the ground mode is eliminated in the II circuit; T i31 and T i41 are the 2P and 2N current components in [ T i ] in the coefficient of the earth mode component.
(5)提取模量:为消除地模分量的影响,采用上述得到的消去地模分量的差模电压、电流分量进行计算。同时进一步考虑到不同极线故障时,各个模量的分布存在差异,由于模量的大小也是故障特征的重要影响因素之一,因此在选择模量参数时,选择较为突出的分量,在此不妨假设为m分量。(5) Extraction modulus: In order to eliminate the influence of the ground mode component, the differential mode voltage and current components obtained above to eliminate the ground mode component are used for calculation. At the same time, it is further considered that the distribution of each modulus is different when different polar faults occur. Since the magnitude of the modulus is also one of the important factors affecting the fault characteristics, when selecting the modulus parameters, choose a more prominent component. Here, we may as well Assumed to be m components.
(6)计算沿线电压分布:根据以上选取的模量,基于贝瑞龙参数模型,根据从两端得到的电压、电流量,采用下式分别计算两端沿线电压的分布:(6) Calculation of voltage distribution along the line: According to the modulus selected above, based on the Berryron parameter model, and according to the voltage and current obtained from both ends, the following formula is used to calculate the distribution of voltage along the line at both ends:
式中:J和K分别表示线路J端和K端;ujn(x,t)表示利用n端电气量计算出的、距离x处的j模电压,n=J、K分别表示直流线路的两端,j=com为模量标号,表示采用差模分量;rm、vm、Zcm分别是m模的电阻率、波速和特征阻抗;m为模量标号,表示采用不同极线故障时较为突出的线模分量。In the formula: J and K represent the J-terminal and K-terminal of the line respectively; u jn (x, t) represents the j-mode voltage at a distance x calculated by using the electrical quantity of the n-terminal, and n=J and K represent the voltage of the DC line respectively At both ends, j=com is the modulus label, indicating that the differential mode component is used; r m , v m , Z cm are the resistivity, wave velocity and characteristic impedance of the m mode respectively; m is the modulus label, indicating that different polar faults are used When the more prominent linear mode component.
(7)构造基于单回信息量的故障定位判据:根据以上构造的消去地模分量的单回相模变换解耦矩阵,选择差模分量进行计算。则可构造故障定位判据如下式:(7) Construct fault location criterion based on single-pass information volume: According to the above-constructed single-pass phase-mode transformation decoupling matrix that eliminates ground-mode components, select differential-mode components for calculation. Then the fault location criterion can be constructed as follows:
式中:uJ(x,t)表示利用J端电气量计算出的、距离J端x处的差模分量电压,x是J端为基准的距离;uK(l-x,t)表示利用K端电气量计算出的、距离K端x处差模电压,x是以J端为基准的距离;t2-t1为所取冗余数据窗的长度,t1为冗余数据窗起始时刻。In the formula: u J (x, t) represents the differential mode component voltage at a distance of x from the J terminal calculated by using the electrical quantity at the J terminal, and x is the distance based on the J terminal; u K (lx, t) indicates that the K Calculated by the terminal electrical quantity, the differential mode voltage at x from terminal K, where x is the distance based on terminal J; t 2 -t 1 is the length of the redundant data window, and t 1 is the start of the redundant data window time.
(8)计算故障时刻:从线路两端计算得到的故障电压行波在非故障点处到达的时间是不同的,所以在故障时刻附近,将存在一个明显的阶跃突变区域,即在理论上具有最大的误差值。若利用该区段进行故障定位,则能够最大限度地放大非故障点的电压差值,从而有利于提高故障点的定位精度,为此不妨将该区段称之为非故障点最大电压差值区段。(8) Calculation of fault time: the arrival time of the fault voltage traveling wave calculated from both ends of the line at non-fault points is different, so there will be an obvious step mutation area near the fault time, that is, in theory has the largest error value. If this section is used for fault location, the voltage difference of non-fault points can be amplified to the greatest extent, which is conducive to improving the positioning accuracy of fault points. For this reason, this section may be called the maximum voltage difference of non-fault points segment.
假设实际故障点距离整流侧的距离为xf,若计算x处的沿线电压分布,则该区段大小ΔT为:Assuming that the distance between the actual fault point and the rectifier side is x f , if the voltage distribution along the line at x is calculated, then the section size ΔT is:
由上式可知,非故障点最大差值区段的大小与偏离故障点的大小成正比,偏离故障点越远,该区域越大,则非故障点电压差值与故障点的差异也越明显,这对于提高测距可靠性显然是非常有利的。It can be known from the above formula that the size of the maximum difference section of the non-fault point is proportional to the size of the deviation from the fault point. The farther away from the fault point, the larger the area, and the more obvious the difference between the voltage difference of the non-fault point and the fault point , which is obviously very beneficial for improving the ranging reliability.
因此采用小波变换获取线路两端行波波头到达时刻,进而求取得到故障时刻,将其作为冗余数据窗的触发时间。Therefore, the wavelet transform is used to obtain the arrival time of the traveling wave head at both ends of the line, and then the fault time is obtained, which is used as the trigger time of the redundant data window.
从线路两端得到的相电压经过相模变换后,取差模分量进行计算。根据小波变换,设置du/dt门槛值以标定两端行波到达时刻,分别设为tR_1、tI_1,若波速为vm,可得到故障初始时刻t0为:After the phase voltage obtained from the two ends of the line is transformed by phase mode, the differential mode component is used for calculation. According to the wavelet transform, set the du/dt threshold value to calibrate the arrival time of traveling waves at both ends, and set them as t R_1 and t I_1 respectively. If the wave velocity is v m , the initial fault time t 0 can be obtained as:
式中:tR_arr为从整流侧计算得到的故障初始时刻;tI_arr为从逆变侧计算得到的故障初始时刻。In the formula: t R_arr is the fault initial time calculated from the rectifier side; t I_arr is the fault initial time calculated from the inverter side.
根据以上分析即可得到故障初始时刻,设为t0,设定所取冗余数据窗的起始时刻,即t1=t0。According to the above analysis, the initial time of the fault can be obtained, set it as t 0 , and set the starting time of the redundant data window, that is, t 1 =t 0 .
(9)确定选取的冗余数据窗:进一步考虑到实际差模分量中所含线模分量的传播速度不同将造成模量行波传播时间存在差异,为更好体现非故障点最大电压差值区段,可以对冗余数据窗的起始时刻增加一定的裕度:(9) Determine the selected redundant data window: further considering that the different propagation speeds of the linear mode components contained in the actual differential mode components will cause differences in the propagation time of the modulus traveling wave, in order to better reflect the maximum voltage difference of the non-fault point Section, you can add a certain margin to the starting time of the redundant data window:
t′1=t0-Δtω,t′ 1 =t 0 -Δt ω ,
式中:t’1为修正后的冗余数据窗的起始时刻;Δtω为所增加的裕度。In the formula: t' 1 is the starting time of the modified redundant data window; Δt ω is the increased margin.
根据以上分析即可确定冗余数据窗。According to the above analysis, the redundant data window can be determined.
本发明的工作原理:本发明的基于单回电气量同塔双回直流输电线路时域故障测距方法是利用构造的消去地模分量的单回相模变换矩阵以得到差模分量,并从线路两端分别计算沿线电压分布,然后根据非故障点的线路两端沿线计算电压在故障时刻附近具有最大差值的特点,定义了非故障点最大电压差值区段,并利用小波变换得到故障初始时刻,确定采用的冗余数据窗从而进行故障测距的方法。Working principle of the present invention: the method for time-domain fault location of double-circuit direct current transmission lines based on single-circuit electrical quantity of the present invention is to use the single-circuit phase-mode transformation matrix constructed to eliminate the ground-mode component to obtain the differential-mode component, and obtain the differential-mode component from the line Calculate the voltage distribution along the line at both ends, and then according to the characteristic that the calculated voltage at both ends of the non-fault point along the line has the largest difference near the fault time, define the maximum voltage difference section of the non-fault point, and use the wavelet transform to obtain the fault initial time, determine the redundant data window to be used for fault location method.
由于同塔双回直流输电线路不仅同一回线存在相间互感,而且不同回线间也存在线间互感,电磁耦合机理复杂,需要对线路进行解耦。由于现有实际工程中的同塔双回直流输电工程各回系统的控制保护是基于本回电气量信息的。但传统单回直流输电线路的相模变换矩阵直接应用于非对称换位的同塔双回直流输电线路具有一定的局限性。并且经过传统单回直流输电线路相模变换得到的差模分量中包含了地模分量和所有的线模分量。由于地模分量受大地电导率和频率的影响很大,对于长距离输电的直流线路,地模分量对于实现准确的故障测距是不利的。因此本发明基于单回线路电气量,根据同塔双回直流输电线路的相模变换矩阵,提出一种消去地模分量的单回相模变换矩阵,进而得到仅含线模分量的差模分量。同时本发明考虑到不同极线故障时,各个模量的分布具有差异性的特点,根据主成分优先原则选择较为突出的线模分量参数,进而得到两端沿线电压分布。最后在根据非故障点的线路两端沿线电压在故障时刻附近具有最大差值的特点,定义了非故障点最大电压差值区段。若利用该区段进行故障定位,则能够最大限度地放大非故障点的电压差值,从而有利于提高故障点的测距精度。因此本发明利用小波变换获取线路两端差模分量行波波头到达时刻,进而求取得到故障时刻,将其作为冗余数据窗的触发时间,从而得到了一种基于单回信息量的同塔双回直流输电线路的故障测距方法。Since the double-circuit DC transmission line on the same tower not only has phase-to-phase mutual inductance in the same circuit, but also has inter-line mutual inductance between different circuits, the electromagnetic coupling mechanism is complex, and the line needs to be decoupled. Because the control and protection of each circuit system of the same-tower double-circuit DC power transmission project in the existing actual project is based on the electrical quantity information of this circuit. However, the direct application of the phase-mode transformation matrix of the traditional single-circuit DC transmission line to the asymmetrically transposed double-circuit DC transmission line on the same tower has certain limitations. And the differential mode component obtained through the phase mode transformation of the traditional single-circuit DC transmission line includes the ground mode component and all the line mode components. Because the ground mode component is greatly affected by the conductivity and frequency of the earth, for the DC line of long-distance power transmission, the ground mode component is unfavorable for realizing accurate fault location. Therefore, the present invention proposes a single-circuit phase-mode transformation matrix that eliminates the ground-mode component based on the electrical quantity of the single-circuit line, and according to the phase-mode transformation matrix of the double-circuit DC transmission line on the same tower, and then obtains the differential mode component containing only the line-mode component. At the same time, the present invention considers that the distribution of each modulus is different when different polar lines are faulted, and selects more prominent line mode component parameters according to the principal component priority principle, and then obtains the voltage distribution along the two ends. Finally, according to the characteristic that the voltage along the line at both ends of the non-fault point has the largest difference near the fault time, the maximum voltage difference section of the non-fault point is defined. If this section is used for fault location, the voltage difference of non-fault points can be amplified to the greatest extent, which is conducive to improving the distance measurement accuracy of fault points. Therefore, the present invention uses wavelet transform to obtain the arrival time of the traveling wave head of the differential-mode component at both ends of the line, and then obtains the fault time, which is used as the trigger time of the redundant data window, thereby obtaining a dual-mode dual-mode component on the same tower based on the amount of single-return information. Fault location method for DC transmission lines.
与现有技术相比,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:
第一、适用于不对称换位的同塔双回直流输电线路故障测距。First, it is suitable for fault location of double-circuit DC transmission lines on the same tower with asymmetric transposition.
第二、基于单回线路电气量信息,与实际工程一致,具有良好的工程应用前景。Second, based on the electrical quantity information of single-circuit lines, it is consistent with actual engineering and has good engineering application prospects.
第三、可靠性高,消去了地模分量的影响,故障精度基本不受故障极线、故障位置和过渡电阻的影响,高阻接地时仍能保证故障测距精度。Third, the reliability is high, the influence of the ground model component is eliminated, the fault accuracy is basically not affected by the fault pole line, fault location and transition resistance, and the fault location accuracy can still be guaranteed when the high resistance is grounded.
第四、故障测距精度高。本发明定义了非故障点最大电压差值区段,最大限度的放大非故障点处的电压差值,更易识别故障点,提高故障测距精度。Fourth, the fault location accuracy is high. The invention defines the maximum voltage difference section of the non-fault point, amplifies the voltage difference at the non-fault point to the greatest extent, makes it easier to identify the fault point, and improves the accuracy of fault distance measurement.
第五、所需数据时窗短,仅需提取线路两端电气量,易于实现。Fifth, the required data time window is short, and only the electrical quantities at both ends of the line need to be extracted, which is easy to implement.
附图说明Description of drawings
图1是本发明的同塔双回直流输电系统模型图。Fig. 1 is a model diagram of the same-tower double-circuit direct current transmission system of the present invention.
图2是本发明的同塔双回直流输电系统杆塔结构图。Fig. 2 is a structure diagram of the pole tower of the same-tower double-circuit direct current transmission system of the present invention.
图3是故障定位图。Figure 3 is a fault location map.
具体实施方式detailed description
下面结合实施例及附图,对本发明作进一步地详细说明,但本发明的实施方式不限于此。The present invention will be described in further detail below in conjunction with the embodiments and the accompanying drawings, but the embodiments of the present invention are not limited thereto.
实施例Example
如图1所示,采用PSCAD/EMTDC仿真软件,构建溪洛渡送电广东±500kV同塔双回直流输电系统模型,其杆塔结构如图2所示;同塔双回双极直流输电线路模型采用依频参数模型,线路全长1254km;设置故障发生于不同位置,故障过渡电阻包括金属性接地和经300Ω过渡电阻接地;故障类型分别包括上层极线故障,下层极线故障以及上下层极线同时故障。该系统利用本发明的故障测距方法,具体包括以下步骤:As shown in Figure 1, the PSCAD/EMTDC simulation software is used to construct the ±500kV same-tower double-circuit HVDC transmission system model in Guangdong for Xiluodu power transmission, and its tower structure is shown in Figure 2; The frequency parameter model, the total length of the line is 1254km; set the fault to occur in different positions, the fault transition resistance includes metallic grounding and grounding through a 300Ω transition resistance; the fault types include the upper polar line fault, the lower polar line fault and the simultaneous fault of the upper and lower polar lines . This system utilizes fault location method of the present invention, specifically comprises the following steps:
S1、提取单位阻抗矩阵和单位导纳矩阵:S1. Extract unit impedance matrix and unit admittance matrix:
根据杆塔的模型得到同塔双回直流输电线路的单位阻抗矩阵[Zphase]和单位导纳矩阵[Yphase]:According to the tower model, the unit impedance matrix [Z phase ] and unit admittance matrix [Y phase ] of the double-circuit DC transmission line on the same tower are obtained:
S2、求取同塔双回直流输电线路相模变换矩阵:S2. Find the phase-mode transformation matrix of the double-circuit DC transmission line on the same tower:
根据得到的单位阻抗矩阵[Zphase]和单位导纳矩阵[Yphase],求取电压解耦矩阵[Tv]、电流解耦矩阵[Ti]:According to the obtained unit impedance matrix [Z phase ] and unit admittance matrix [Y phase ], the voltage decoupling matrix [T v ] and the current decoupling matrix [T i ] are obtained:
根据上述式子可以得到:According to the above formula can get:
S3、构造消去地模分量的单回电压相模变换矩阵:S3. Construct a single-circuit voltage phase-mode transformation matrix that eliminates the ground-mode component:
根据以上得到的电压解耦矩阵[Tv],求出同塔双回直流输电线路测量端的各模量电压瞬时值,其中0表示地模分量,1、2和3表示第一线模分量、第二线模分量和第三线模分量,则各极的电压量可以表示为:According to the voltage decoupling matrix [T v ] obtained above, the instantaneous value of each modulus voltage at the measuring end of the double-circuit DC transmission line on the same tower is obtained, where 0 represents the ground mode component, 1, 2 and 3 represent the first line mode component, The second linear mode component and the third linear mode component, then the voltage of each pole can be expressed as:
对于I回线路,新的单回变换矩阵形式为:For the I-circuit line, the new single-circuit transformation matrix form is:
则经过消去地模分量的单回变换矩阵后得到的I回线路的差模电压分量为:Then the differential-mode voltage component of the I-circuit line obtained after eliminating the single-circuit transformation matrix of the ground-mode component is:
Udif_I_eli0=-0.1861u1+0.4494u2+0.4830u3,U dif_I_eli0 =-0.1861u 1 +0.4494u 2 +0.4830u 3 ,
对于II回线路,新的单回变换矩阵形式为:For circuit II, the form of the new single-circuit transformation matrix is:
则经过消去地模分量的单回变换矩阵后得到的II回线路的差模电压分量为:Then the differential-mode voltage component of the II-circuit line obtained after eliminating the single-circuit transformation matrix of the ground-mode component is:
Udif_II_eli0=-0.1861u1+0.4494u2+0.4830u3,U dif_II_eli0 = -0.1861u 1 +0.4494u 2 +0.4830u 3 ,
S4、构造消去地模分量的单回电流相模变换矩阵:S4. Construct a single-circuit current phase-mode transformation matrix that eliminates the ground-mode component:
根据以上得到的电流解耦矩阵[Ti],求出同塔双回直流输电线路测量端的各模量电流瞬时值,其中0表示地模分量,1、2和3表示第一线模分量、第二线模分量和第三线模分量,则各极的电流量可以表示为:According to the current decoupling matrix [T i ] obtained above, the instantaneous value of each modulus current at the measurement end of the double-circuit DC transmission line on the same tower is obtained, where 0 represents the ground mode component, 1, 2 and 3 represent the first line mode component, The second linear mode component and the third linear mode component, then the current of each pole can be expressed as:
对于I回线路,新的单回变换矩阵形式为:For the I-circuit line, the new single-circuit transformation matrix form is:
则经过消去地模分量的单回变换矩阵后得到的I回线路的差模电流分量为:Then the differential-mode current component of the I-circuit line obtained after eliminating the single-circuit transformation matrix of the ground-mode component is:
Idif_I_eli0=-0.0999i1+0.5150i2+0.5178i3,I dif_I_eli0 =-0.0999i 1 +0.5150i 2 +0.5178i 3 ,
对于II回线路,新的单回变换矩阵形式为:For circuit II, the form of the new single-circuit transformation matrix is:
则经过消去地模分量的单回变换矩阵后得到的I回线路的差模电流分量为:Then the differential-mode current component of the I-circuit line obtained after eliminating the single-circuit transformation matrix of the ground-mode component is:
Idif_II_eli0=-0.0999i1+0.5150i2+0.5178i3,I dif_II_eli0 =-0.0999i 1 +0.5150i 2 +0.5178i 3 ,
S5、针对不同极线故障时各个线模分量的分布特点,选取较为突出的分量。由于线模3分量较为突出,因此模量参数选择线模3对应参数。S5. According to the distribution characteristics of each line mode component when different polar faults occur, a more prominent component is selected. Since the component of line mode 3 is more prominent, the corresponding parameter of line mode 3 is selected for the modulus parameter.
S6、计算沿线电压分布:S6. Calculate the voltage distribution along the line:
计算两端沿线电压分布。使用下式:Calculate the voltage distribution along the line at both ends. Use the following formula:
其中,J和K分别表示线路J端和K端;ujn(x,t)表示利用n端电气量计算出的、距离x处的j模电压,n=J、K分别表示直流线路的两端,j=com为模量标号,表示采用差模分量;r3、v3、Zc3分别是3模对应的的电阻率、波速和特征阻抗。Among them, J and K represent the J-terminal and K-terminal of the line respectively; u jn (x, t) represents the j-mode voltage at a distance x calculated by using the electrical quantity of the n-terminal, and n=J and K represent the two sides of the DC line respectively. At the end, j=com is the modulus label, indicating that the differential mode component is used; r 3 , v 3 , and Z c3 are the resistivity, wave velocity, and characteristic impedance corresponding to the three modes, respectively.
S7、故障定位:S7. Fault location:
根据以上构造的消去地模分量的单回相模变换解耦矩阵,选择差模分量进行计算。则可构造故障定位判据如下式:According to the single-phase phase-mode transformation decoupling matrix constructed above to eliminate the ground-mode component, the differential-mode component is selected for calculation. Then the fault location criterion can be constructed as follows:
其中,uJ(x,t)表示利用J端电气量计算出的、距离J端x处的差模分量电压,x是J端为基准的距离;uK(l-x,t)表示利用K端电气量计算出的、距离K端x处差模电压,x是以J端为基准的距离;t2-t1为所取冗余数据窗的长度。Among them, u J (x, t) represents the differential mode component voltage at a distance of x from the J terminal calculated by using the electrical quantity of the J terminal, and x is the distance based on the J terminal; u K (lx, t) indicates that using the K terminal The differential mode voltage calculated from the electrical quantity at x from terminal K, where x is the distance based on terminal J; t 2 -t 1 is the length of the redundant data window.
S8、计算故障初始时刻:S8. Calculate the initial moment of failure:
根据小波变换,设置du/dt门槛值以标定两端行波到达整流侧和逆变侧的时刻,分别设为tR_1、tI_1,波速为v3,可得到故障初始时刻t0为:According to the wavelet transform, set the du/dt threshold value to calibrate the time when the traveling waves at both ends reach the rectification side and the inverter side, respectively set t R_1 , t I_1 , and the wave velocity is v 3 , the initial time t 0 of the fault can be obtained as:
式中,tR_arr为从整流侧计算得到的故障初始时刻;tI_arr为从逆变侧计算得到的故障初始时刻。In the formula, t R_arr is the fault initial time calculated from the rectifier side; t I_arr is the fault initial time calculated from the inverter side.
根据以上分析即可得到故障初始时刻,设为t0,设定所取冗余数据窗的触发时刻,即t1=t0。According to the above analysis, the initial time of the fault can be obtained, set it as t 0 , and set the trigger time of the redundant data window, that is, t 1 =t 0 .
S9、冗余数据窗的选取:S9. Selection of redundant data windows:
为了保证更好识别沿线电压差异最大点,可以对冗余数据窗的触发时刻增加一定的裕度:In order to better identify the point with the largest voltage difference along the line, a certain margin can be added to the triggering time of the redundant data window:
t′1=t0-Δtω,t′ 1 =t 0 -Δt ω ,
式中,t’1为修正后的冗余数据窗的触发时刻;Δtω为所增加的裕度,取0.2ms。In the formula, t' 1 is the trigger time of the modified redundant data window; Δt ω is the increased margin, which is 0.2ms.
如图3所示,为距离整流侧100km处Ⅱ回线路负极发生金属性接地故障时的定位结果。As shown in Figure 3, it is the location result when a metallic ground fault occurs at the negative pole of the second circuit line at a distance of 100km from the rectifier side.
如以下的表1所示,列出了在Ⅱ回线路故障发生不同位置、经过不同过渡电阻接地的故障定位结果。As shown in Table 1 below, the fault location results of different locations where the fault occurs in the second circuit line and grounded through different transition resistances are listed.
表1Table 1
由表1的故障定位结果可知,本发明所提的故障测距方法是准确有效的,能够实现线路全长范围内的准确测距,且测距精度不受故障极线,故障位置和过渡电阻的影响。From the fault location results in Table 1, it can be seen that the fault location method proposed in the present invention is accurate and effective, and can achieve accurate distance measurement within the entire length of the line, and the distance measurement accuracy is not affected by the fault pole line, fault location and transition resistance. Impact.
上述实施例为本发明较佳的实施方式,但本发明的实施方式并不受所述实施例的限制,其他的任何未背离本发明的精神实质与原理下所作的改变、修饰、替代、组合、简化,均应为等效的置换方式,都包含在本发明的保护范围之内。The above-mentioned embodiment is a preferred embodiment of the present invention, but the embodiment of the present invention is not limited by the embodiment, and any other changes, modifications, substitutions and combinations made without departing from the spirit and principle of the present invention , simplification, all should be equivalent replacement methods, and are all included in the protection scope of the present invention.
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| CN108092244A (en) * | 2017-12-15 | 2018-05-29 | 华南理工大学 | A kind of common-tower double-return HVDC transmission line traveling-wave protection method |
| CN108445354A (en) * | 2018-05-23 | 2018-08-24 | 南方电网科学研究院有限责任公司 | Fault location method, device, equipment and medium based on traveling wave difference current |
| CN112415433A (en) * | 2019-08-21 | 2021-02-26 | 华东师范大学 | Long-lead short-circuit fault point positioning device and method |
| CN112595929A (en) * | 2020-12-09 | 2021-04-02 | 天津大学 | Monopole grounding fault location method suitable for true bipolar flexible direct system |
| CN113064023A (en) * | 2021-03-18 | 2021-07-02 | 电子科技大学 | A method and system for fault identification of multi-circuit transmission lines on the same tower |
| CN113156259A (en) * | 2021-02-22 | 2021-07-23 | 天津大学 | Flexible direct-current power grid double-end fault location method based on Marti frequency-variable model |
| CN115980514A (en) * | 2023-02-20 | 2023-04-18 | 国网湖北省电力有限公司武汉供电公司 | A fault location method for complex distribution network based on multi-terminal traveling wave frequency matrix |
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| CN120703505A (en) * | 2025-08-27 | 2025-09-26 | 国网陕西省电力有限公司电力科学研究院 | A method and related equipment for measuring mutual inductance parameters of double-circuit transmission lines on the same tower |
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Cited By (13)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108092244A (en) * | 2017-12-15 | 2018-05-29 | 华南理工大学 | A kind of common-tower double-return HVDC transmission line traveling-wave protection method |
| CN108445354A (en) * | 2018-05-23 | 2018-08-24 | 南方电网科学研究院有限责任公司 | Fault location method, device, equipment and medium based on traveling wave difference current |
| CN108445354B (en) * | 2018-05-23 | 2020-05-08 | 南方电网科学研究院有限责任公司 | Fault location method, device, equipment and medium based on traveling wave differential current |
| CN112415433A (en) * | 2019-08-21 | 2021-02-26 | 华东师范大学 | Long-lead short-circuit fault point positioning device and method |
| CN112595929A (en) * | 2020-12-09 | 2021-04-02 | 天津大学 | Monopole grounding fault location method suitable for true bipolar flexible direct system |
| CN112595929B (en) * | 2020-12-09 | 2022-08-02 | 天津大学 | Monopole grounding fault location method suitable for true bipolar flexible direct system |
| CN113156259A (en) * | 2021-02-22 | 2021-07-23 | 天津大学 | Flexible direct-current power grid double-end fault location method based on Marti frequency-variable model |
| CN113064023B (en) * | 2021-03-18 | 2022-01-04 | 电子科技大学 | A method and system for fault identification of multi-circuit transmission lines on the same tower |
| CN113064023A (en) * | 2021-03-18 | 2021-07-02 | 电子科技大学 | A method and system for fault identification of multi-circuit transmission lines on the same tower |
| CN115980514A (en) * | 2023-02-20 | 2023-04-18 | 国网湖北省电力有限公司武汉供电公司 | A fault location method for complex distribution network based on multi-terminal traveling wave frequency matrix |
| CN120507688A (en) * | 2025-04-07 | 2025-08-19 | 国家电网有限公司华东分部 | Method, device, medium and computer equipment for detecting faults of same-tower non-transposition line |
| CN120703505A (en) * | 2025-08-27 | 2025-09-26 | 国网陕西省电力有限公司电力科学研究院 | A method and related equipment for measuring mutual inductance parameters of double-circuit transmission lines on the same tower |
| CN120703505B (en) * | 2025-08-27 | 2025-11-18 | 国网陕西省电力有限公司电力科学研究院 | A method and related equipment for measuring mutual inductance parameters of a double-circuit transmission line on the same tower. |
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