CN103941091A - Power system HHT harmonious wave detection method based on improved EMD end point effect - Google Patents
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Abstract
本发明涉及电力系统谐波检测领域,特别是一种基于改进EMD端点效应的电力系统HHT谐波检测方法。该方法针对EMD分解过程中出现的信号边界失真现象,通过选取端点和极值点作为参考变量,对端点和极值点的关系进行比较,采用镜像延拓的方法对端点效应进行改进,并利用改进之后的镜像法对电力系统谐波进行EMD分解,得到所有的固有模态函数(IMF),利用Hilbert变换对经过EMD分解之后的电力系统谐波分解得到信号的时频特性。该方法有利于快速检测出电力系统谐波中的谐波组成,从而提高电力系统谐波辨识能力,适用于电力系统等相关部门,用于电力系统谐波检测。
The invention relates to the field of harmonic detection in electric power systems, in particular to an HHT harmonic detection method in electric power systems based on improved EMD endpoint effects. Aiming at the phenomenon of signal boundary distortion in the process of EMD decomposition, this method compares the relationship between endpoints and extreme points by selecting endpoints and extreme points as reference variables, and uses the method of mirror extension to improve the effect of endpoints. The improved image method decomposes the harmonics of the power system by EMD to obtain all the intrinsic mode functions (IMF), and uses the Hilbert transform to decompose the harmonics of the power system after EMD decomposition to obtain the time-frequency characteristics of the signal. This method is beneficial to quickly detect the harmonic composition in the harmonics of the power system, thereby improving the harmonic identification ability of the power system, and is suitable for relevant departments such as the power system for the harmonic detection of the power system.
Description
技术领域 technical field
本发明涉及电力系统谐波检测领域,特别是一种基于改进EMD端点效应的电力系统HHT谐波检测方法。 The invention relates to the field of harmonic detection in electric power systems, in particular to an HHT harmonic detection method in electric power systems based on improved EMD endpoint effects.
背景技术 Background technique
电力系统谐波是电力质量的重要指标之一,谐波的存在直接影响到电力用户的正常用电。对电力系统谐波进行检测是处理电力系统谐波问题的基础,为保证高质量的供电,必须对电力系统谐波进行检测。 Power system harmonics are one of the important indicators of power quality, and the existence of harmonics directly affects the normal power consumption of power users. The detection of power system harmonics is the basis for dealing with power system harmonics. In order to ensure high-quality power supply, it is necessary to detect power system harmonics.
目前,常用的电力系统谐波检测方法主要有模拟滤波器法、基于瞬时无功功率的谐波检测法、基于傅里叶变换的谐波检测法以及基于小波变换的谐波检测法等几种方法。模拟滤波器电路实现容易、成本低,但是易受环境影响,检测精度不能保证;基于无功功率理论的谐波检测方法能够精确检测谐波,检测电路比较简单,但是在用低通滤波器提取直流分量时,会有一个电源周期的延时;基于快速傅氏变换(FFT)检测法的优点是可以选择拟消除的谐波次数,缺点是延时较长,实时性稍差;小波变换虽然能将信号在不同尺度下进行多分辨分解,但小波变换本质是一种基于基函数展开的理论,信号分析很大程度上依赖基函数的选择,而对一个具体问题而言,最优基的选择没有确定的规则可循,造成分析不理想,只适合瞬态和非平稳信号。 At present, the commonly used harmonic detection methods in power systems mainly include analog filter method, harmonic detection method based on instantaneous reactive power, harmonic detection method based on Fourier transform, and harmonic detection method based on wavelet transform. method. The analog filter circuit is easy to implement and low in cost, but it is easily affected by the environment, and the detection accuracy cannot be guaranteed; the harmonic detection method based on reactive power theory can accurately detect harmonics, and the detection circuit is relatively simple, but the low-pass filter is used to extract When there is a DC component, there will be a delay of a power cycle; the advantage of the fast Fourier transform (FFT) detection method is that the harmonic order to be eliminated can be selected, but the disadvantage is that the delay is long and the real-time performance is slightly poor; although the wavelet transform The signal can be decomposed into multi-resolution at different scales, but the essence of wavelet transform is a theory based on the expansion of basis functions. Signal analysis largely depends on the selection of basis functions, and for a specific problem, the optimal basis There is no definite rule to follow for the selection, which makes the analysis not ideal, and is only suitable for transient and non-stationary signals.
希尔伯特-黄(HHT)算法是在1998年由美籍华人黄锷(Norden E.Huang)提出的,该算法是一种新型的时频分析方法,解决了原有时频分析方法的不足之处,适用于非线性非平稳信号的处理, 自提出之后就在各领域得到了广泛的应用。HHT算法先用经验模态分解方法(EMD)获得有限数目的固有模态函数(Intrinsic Mode Function,简称IMF),然后再利用Hilbert变换和瞬时频率方法获得信号的时域频谱。但在边界处理、模态混叠和曲线拟合等方面还存在缺陷与不足,从而影响了HHT的分析效果,需要对其进行优化和改进。因此,本发明在综合比较了各种电力系统谐波检测的方法后,采用了HHT算法对电力系统谐波进行检测,并在原有算法的基础上,选择边界处理为出发点,对EMD端点效应进行改进。并应用于电力系统谐波检测,不仅对希尔伯特-黄变换的研究和推广有重要意义,也是与电力系统谐波检测相结合的有益探索。 The Hilbert-Huang (HHT) algorithm was proposed by Norden E. Huang, a Chinese-American in 1998. This algorithm is a new type of time-frequency analysis method, which solves the shortcomings of the original time-frequency analysis method. It is suitable for the processing of nonlinear and non-stationary signals, and has been widely used in various fields since it was proposed. The HHT algorithm first uses the empirical mode decomposition method (EMD) to obtain a limited number of intrinsic mode functions (IMF for short), and then uses the Hilbert transform and the instantaneous frequency method to obtain the time domain spectrum of the signal. However, there are still defects and deficiencies in boundary processing, mode mixing and curve fitting, which affect the analysis effect of HHT, and need to be optimized and improved. Therefore, the present invention adopts the HHT algorithm to detect the harmonics of the power system after comprehensively comparing various methods for detecting the harmonics of the power system, and on the basis of the original algorithm, selects the boundary processing as the starting point, and conducts the EMD endpoint effect Improve. And it is applied to the harmonic detection of the power system, which is not only of great significance to the research and promotion of the Hilbert-Huang transform, but also a beneficial exploration combined with the harmonic detection of the power system.
发明内容 Contents of the invention
本发明的目的在于提供一种基于改进EMD端点效应的电力系统HHT谐波检测方法,该方法有利于提高对电力系统谐波的检测,从而提高谐波辨识能力。 The purpose of the present invention is to provide a power system HHT harmonic detection method based on the improved EMD endpoint effect, which is conducive to improving the detection of power system harmonics, thereby improving the ability of harmonic identification.
为实现上述目的,本发明的技术方案是:一种基于改进EMD端点效应的电力系统HHT谐波检测方法,采用镜像延拓的方法对端点效应进行改进,利用改进之后的镜像法对电力系统谐波进行EMD分解,并利用Hilbert变换对经过EMD分解之后的电力系统谐波分解得到该谐波信号的时频特性,其具体步骤如下: In order to achieve the above object, the technical solution of the present invention is: a power system HHT harmonic detection method based on the improved EMD endpoint effect, using the method of mirror extension to improve the endpoint effect, and using the improved mirror image method to detect the harmonic of the power system The wave is decomposed by EMD, and the time-frequency characteristics of the harmonic signal are obtained by using the Hilbert transform to decompose the harmonics of the power system after EMD decomposition. The specific steps are as follows:
步骤S1:选取极值点和端点值为参数变量,定义 k为固有模态函数迭代次数,k=0,1,2,···n;m为固有模态函数阶数,m=1,2,3···n;选取经过滤波之后的电力系统谐波信号 进行分析; Step S1: Select extreme points and endpoints as parameter variables, define k as the number of iterations of the intrinsic mode function, k=0,1,2,...n; m is the order of the intrinsic mode function, m=1, 2,3···n; select the harmonic signal of the power system after filtering to analyze;
步骤S2:令剩余分量,如果是单调函数,则输出结果,否则转步骤S3; Step S2: Let the remaining components ,if is a monotone function, then output the result, otherwise go to step S3;
步骤S3:对电力系统谐波进行分析,首先获取极大值点时间序列、极小值点时间序列、左端点值和右端点值,然后采用镜面选取原则确定左镜面以及右镜面的放置位置;其中,和表示极值点在整个电力系统谐波信号数据中极值点出现的时间顺序序列,i=0,1,2,···n; Step S3: Harmonics of the power system For analysis, first obtain the time series of maximum points , time series of minimum points , left endpoint value and the right endpoint value , and then use the mirror selection principle to determine the placement positions of the left mirror and the right mirror; among them, and Indicates the chronological sequence of extreme points appearing in the harmonic signal data of the entire power system, i =0,1,2,...n;
步骤S4:利用放置好的镜面对电力系统谐波信号进行镜像延拓,左右端部根据镜面选取原则分别延拓一个周期; Step S4: Use the placed mirror to perform mirror extension on the harmonic signal of the power system, and the left and right ends are respectively extended for one cycle according to the principle of mirror selection;
步骤S5:对左右端部分分别经过镜像延拓一个周期之后的电力系统谐波信号,根据三次样条插值法对其进行包络,得到上下包络线,分别记为和;取包络线的均值,并计算包络线均值与电力系统谐波信号的差; Step S5: Envelope the harmonic signals of the power system after the left and right ends have been mirrored and extended for one period respectively according to the cubic spline interpolation method to obtain the upper and lower envelopes, which are denoted as and ; Take the mean value of the envelope , and calculate the mean value of the envelope and power system harmonic signals the difference ;
步骤S6:对进行IMF判定,如果满足如下条件: Step S6: Yes Carry out IMF judgment, if Meet the following conditions:
(1)极值点和过零点的数目应该相等或至多差一个; (1) The number of extreme points and zero-crossing points should be equal or at most one difference;
(2)分别连接其局部最大值和局部最小值所形成的包络线的均值在任意一点处为零,即信号关于时间轴局部对称; (2) The mean value of the envelope formed by connecting its local maximum and local minimum is zero at any point, that is, the signal is locally symmetrical about the time axis;
则将作为电力系统谐波信号的第一个IMF分量,否则将作为新的电力系统谐波信号,转步骤S3,并重复k次,得到,利用的值来判断每次筛选结果是否满足IMF条件: then will Harmonic signal of power system The first IMF component of , otherwise it will be As a new power system harmonic signal, go to step S3 and repeat k times to get ,use value to determine whether each screening result meets the IMF condition:
式中,为对重复次所得的分量,的取值范围通常在0.2~0.3;满足的要求时,则将作为电力系统谐波信号的第一阶IMF分量,记为,将从电力系统谐波信号中分离出来得到剩余分量: In the formula, for right repeat The amount of time obtained, The value range of is usually 0.2~0.3; satisfy When requested, the As the first-order IMF component of the power system harmonic signal, denoted as ,Will Harmonic signals from power systems Separated from to get the remaining components:
式中,是分解出第一阶IMF分量之后的剩余分量; In the formula, is the remaining component after decomposing the first-order IMF component;
步骤S7:将作为新的电力系统谐波信号,重复步骤S3-S6,直到最终剩余分量为一个常量或者是一个单调函数,于是电力系统谐波信号的EMD分解结果可以表示为: Step S7: put As a new power system harmonic signal , repeat steps S3-S6 until the final remaining component is a constant or a monotonic function, so the EMD decomposition result of the power system harmonic signal can be expressed as:
上式中,为电力系统谐波EMD分解完成之后的IMF分量,m为IMF分量阶数; In the above formula, is the IMF component after the power system harmonic EMD decomposition is completed, and m is the order of the IMF component;
步骤S8:EMD分解完成后,对电力系统谐波进行时频分析,首先,对EMD分解得到的任意一阶IMF分量进行Hilbert变换,则: Step S8: After the EMD decomposition is completed, time-frequency analysis is performed on the harmonics of the power system. First, the Hilbert transform is performed on any first-order IMF component obtained from the EMD decomposition, then:
上式中,是的Hilbert变换; In the above formula, yes Hilbert transform;
步骤S9:定义的解析信号: Step S9: Define The parsed signal:
式中,即为的解析信号; In the formula, that is analysis signal;
步骤S10:根据解析信号求解IMF分量的瞬时幅值、瞬时相位和瞬时频率: Step S10: Solve the instantaneous amplitude, instantaneous phase and instantaneous frequency of the IMF component according to the analytical signal:
上式中,、和分别表示瞬时幅值、瞬时相位和瞬时频率;至此,由步骤S9-S10 In the above formula, , and represent the instantaneous amplitude, instantaneous phase and instantaneous frequency respectively; so far, by steps S9-S10
求出任意一阶固有模态函数瞬时功率、瞬时相位和瞬时频率; Calculate the instantaneous power, instantaneous phase and instantaneous frequency of any first-order intrinsic mode function;
步骤S11:求出瞬时功率、瞬时相位和瞬时频率之后,继续求解Hilbert谱;省略剩余分量,并定义Hilbert谱,记作: Step S11: After calculating the instantaneous power, instantaneous phase and instantaneous frequency, continue to solve the Hilbert spectrum; omit the remaining components , and define the Hilbert spectrum, denoted as:
上式中,; In the above formula, ;
步骤S12:进一步求解Hilbert边际谱,记作: Step S12: Further solve the Hilbert marginal spectrum, denoted as:
Hilbert边际谱提供了每一个频率值上分布的总的振幅和能量,它以概率的形式表示在整个数据序列上的累计振幅或能量;至此,利用改进EMD端点效应的HHT对电力系统谐波信号完成检测分析。 The Hilbert marginal spectrum provides the total amplitude and energy distributed on each frequency value, which expresses the cumulative amplitude or energy on the entire data sequence in the form of probability; so far, the HHT of the improved EMD endpoint effect is used for power system harmonic signals Complete assay analysis.
在本发明实施例中,在步骤S3中,所述镜面选取原则具体如下, In the embodiment of the present invention, in step S3, the mirror surface selection principle is specifically as follows,
对左边的极值点与左端点值相比较确定左镜面的放置位置,对右边的极值点与右端点值进行比较确定右镜面的放置位置;则, Compare the left extreme point with the left endpoint value to determine the placement position of the left mirror, and compare the right extreme point with the right endpoint value to determine the placement position of the right mirror; then,
左端镜面时间序列: Left end mirror time series:
谐波信号初始递增时: When the harmonic signal is initially incremented:
谐波信号初始递减时: When the harmonic signal initially decreases:
右端镜面时间序列: Right-hand mirror time series:
谐波信号末尾递增时: When increasing at the end of the harmonic signal:
谐波信号末尾递减时: When the end of the harmonic signal decreases:
式中,、分别为左端镜面时间序列和右端镜面时间序列,左、右端镜面时间序列为1 或n时,表示将镜面放置在左端点处或右端点处,、、和分别表示信号序列左极大值、左极小值、右极大值和右极小值。 In the formula, , are the left end mirror time series and the right end mirror time series respectively, when the left and right end mirror time series are 1 or n, it means that the mirror is placed at the left end or right end, , , and Represents the left maximum, left minimum, right maximum and right minimum of the signal sequence, respectively.
在本发明实施例中,在步骤S4中,经过镜像延拓之后的极小值和极大值时间序列分别为: In the embodiment of the present invention, in step S4, the minimum value and maximum value time series after mirror extension They are:
式中,和分别为延拓后的左极小值、左极大值、右极小值和右极大值时间序列,为原极值点延拓之后的时间序列; In the formula, and are the time series of left minimum, left maximum, right minimum and right maximum, respectively, after continuation, is the time series after the extension of the original extremum point;
经过镜像延拓之后的极小值和极大值序列: The sequence of minima and maxima after mirror continuation:
式中,分别为延拓后的左极小值、左极大值、右极小值和右极大值序列,为原极值点延拓之后的序列。 In the formula, are respectively the extended left minimum value, left maximum value, right minimum value and right maximum value sequence, is the sequence after the extension of the original extremum point.
相较于现有技术,本发明具有以下有益效果: Compared with the prior art, the present invention has the following beneficial effects:
1、端点“飞翼”现象得到了有效的抑制,信号曲线得到了完整的包络; 1. The "flying wing" phenomenon at the endpoint has been effectively suppressed, and the signal curve has obtained a complete envelope;
2、谐波信号能被准确的自适应分离出来,没有了多余的IMF分量,精度得到了很大的提高。 2. Harmonic signals can be accurately and adaptively separated, and there is no redundant IMF component, and the accuracy has been greatly improved.
附图说明 Description of drawings
图1 是本发明实施例的工作流程图。 Fig. 1 is the work flowchart of the embodiment of the present invention.
图2是镜像法进行改进之前的信号包络效果图和原始信号与上下包络线均值之差的效果图。 Figure 2 is an effect diagram of the signal envelope before the mirror method is improved and an effect diagram of the difference between the original signal and the mean value of the upper and lower envelopes.
图3是镜像法进行改进之前对电力系统谐波进行EMD分解的效果图。 Figure 3 is an effect diagram of EMD decomposition of power system harmonics before the improvement of the image method.
图4是镜像法进行改进之前对电力系统谐波求得的瞬时频率和瞬时幅值。 Figure 4 is the instantaneous frequency and instantaneous amplitude obtained for power system harmonics before the improvement of the image method.
图5是镜像法进行改进之前对电力系统谐波求解得到的Hilbert谱。 Figure 5 is the Hilbert spectrum obtained by solving the harmonics of the power system before the image method is improved.
图6是镜像法进行改进之前对电力系统谐波求解得到的Hilbert边际谱。 Figure 6 is the Hilbert marginal spectrum obtained by solving the harmonics of the power system before the improvement of the image method.
图7是镜像法进行改进之后的信号包络效果图和原始信号与上下包络线均值之差的效果图。 Fig. 7 is an effect diagram of the signal envelope after the mirror method is improved and an effect diagram of the difference between the original signal and the mean value of the upper and lower envelopes.
图8是镜像法进行改进之后对电力系统谐波进行EMD分解的效果图。 Figure 8 is an effect diagram of EMD decomposition of power system harmonics after the mirror image method is improved.
图9是镜像法进行改进之后对电力系统谐波求得的瞬时频率和瞬时幅值。 Figure 9 shows the instantaneous frequency and instantaneous amplitude obtained for power system harmonics after the image method is improved.
图10是镜像法进行改进之后对电力系统谐波求解得到的Hilbert谱。 Figure 10 is the Hilbert spectrum obtained by solving the harmonics of the power system after the image method is improved.
图11是镜像法进行改进之后对电力系统谐波求解得到的Hilbert边际谱。 Figure 11 is the Hilbert marginal spectrum obtained by solving the harmonics of the power system after the image method is improved.
具体实施方式 Detailed ways
下面结合附图,对本发明的技术方案进行具体说明。 The technical solution of the present invention will be specifically described below in conjunction with the accompanying drawings.
本发明是一种基于改进EMD端点效应的电力系统HHT谐波检测方法,采用镜像延拓的方法对端点效应进行改进,利用改进之后的镜像法对电力系统谐波进行EMD分解,并利用Hilbert变换对经过EMD分解之后的电力系统谐波分解得到该谐波信号的时频特性; The invention is a power system HHT harmonic detection method based on the improved EMD endpoint effect. The endpoint effect is improved by the method of image continuation, and the EMD decomposition of the power system harmonic is carried out by using the improved image method, and the Hilbert transformation is used. The time-frequency characteristics of the harmonic signal are obtained by decomposing the harmonics of the power system after EMD decomposition;
该电力系统HHT谐波检测方法结合图1进行说明,并对电力系统谐波信号利用改进前和改进后的镜像法进行仿真得到效果图示于附图2-11,具体按如下步骤进行: The power system HHT harmonic detection method is described in conjunction with Figure 1, and the power system harmonic signal Use the pre-improved and improved mirroring method to simulate the effect diagram shown in Figure 2-11, specifically follow the steps below:
步骤1:选取极值点和端点值为参数变量,定义k为固有模态函数迭代次数,k=0,1,2,···n;m为固有模态函数阶数,m=1,2,3···n;选取经过滤波之后的电力系统谐波信号进行分析。 Step 1: Select extreme points and endpoints as parameter variables, define k as the number of iterations of the intrinsic mode function, k=0,1,2,...n; m is the order of the intrinsic mode function, m=1, 2,3···n; select the harmonic signal of the power system after filtering for analysis.
步骤2:令剩余分量,如果是单调函数,则输出结果,否则转步骤3。 Step 2: Make the remaining components ,if is a monotone function, then output the result, otherwise go to step 3.
步骤3:对电力系统谐波进行分析,首先获取极大值点时间序列、极小值点时间序列、左端点值和右端点值,并对左边的极值点与左端点值相比较确定左镜面位置的放置,右边的极值点与右端点值进行比较确定右镜面的放置,其中和表示极值点在整个电力系统谐波信号数据中极值点出现的时间顺序序列,分别用、、和表示信号序列左极大值、左极小值、右极大值和极小值,镜面选取原则可以细化如下: Step 3: For Power System Harmonics For analysis, first obtain the time series of maximum points , time series of minimum points , left endpoint value and the right endpoint value , and compare the extreme point on the left with the value of the left endpoint to determine the placement of the left mirror, and compare the extreme point on the right with the value of the right endpoint to determine the placement of the right mirror, where and Indicates the chronological sequence of extreme points appearing in the harmonic signal data of the entire power system, respectively using , , and Represents the left maximum value, left minimum value, right maximum value and minimum value of the signal sequence, and the mirror selection principle can be refined as follows:
左端镜面时间序列: Left end mirror time series:
谐波信号初始递增时: When the harmonic signal is initially incremented:
谐波信号初始递减时: When the harmonic signal initially decreases:
右端镜面时间序列: Right-hand mirror time series:
谐波信号末尾递增时: When increasing at the end of the harmonic signal:
谐波信号末尾递减时: When the end of the harmonic signal decreases:
式中,、分别为左端镜面时间序列和右端镜面时间序列,左、右端镜面时间序列为1或n时,表示将镜面放置在左端点处或右端点处。 In the formula, , They are the left end mirror time series and the right end mirror time series respectively. When the left and right end mirror time series are 1 or n, it means that the mirror is placed at the left end or right end.
步骤4:利用放置好的镜面对电力系统谐波信号进行镜像延拓。左右端部根据镜面选取原则分别延拓一个周期,经过镜像延拓之后的极小值和极大值时间序列分别为: Step 4: Use the placed mirror to mirror and extend the harmonic signal of the power system. The left and right ends are respectively extended for one cycle according to the principle of mirror surface selection, and the time series of minimum and maximum values after mirror extension They are:
式中,和分别为延拓后的左极小值、左极大值、右极小值和右极大值时间序列,为原极值点延拓之后的时间序列,经过镜像延拓之后的极小值和极大值序列: In the formula, and are the time series of left minimum, left maximum, right minimum and right maximum, respectively, after continuation, is the time series after the continuation of the original extreme point, and the minimum and maximum value series after the mirror continuation:
式中,为经过镜像延拓之后的极小值和极大值序列,分别为延拓后的左极小值、左极大值、右极小值和右极大值序列,为原极值点延拓之后的序列。 In the formula, is the sequence of minima and maxima after mirror extension, are respectively the extended left minimum value, left maximum value, right minimum value and right maximum value sequence, is the sequence after the extension of the original extremum point.
步骤5:对经过镜像左右端部分分别延拓一个周期之后的电力系统谐波信号,根据三次样条插值法对其进行包络,得到上下包络线,分别记为和。取包络线的均值,并计算包络线均值与电力系统谐波信号的差。 Step 5: Envelope the harmonic signal of the power system after the left and right ends of the mirror image have been extended for one period respectively according to the cubic spline interpolation method to obtain the upper and lower envelopes, which are denoted as and . Take the mean of the envelope , and calculate the mean value of the envelope and power system harmonic signals the difference .
步骤6:对进行IMF判定,如果满足如下条件: Step 6: Right Carry out IMF judgment, if Meet the following conditions:
(1)极值点和过零点的数目应该相等或至多差一个; (1) The number of extreme points and zero-crossing points should be equal or at most one difference;
(2)分别连接其局部最大值和局部最小值所形成的包络线的均值在任意一点处为零,即信号关于时间轴局部对称; (2) The mean value of the envelope formed by connecting its local maximum and local minimum is zero at any point, that is, the signal is locally symmetrical about the time axis;
则将作为电力系统谐波信号的第一个IMF分量,否则将作为新的电力系统谐波信号,转步骤3,并重复k次,得到,利用的值来判断每次筛选结果是否满足IMF条件: then will Harmonic signal of power system The first IMF component of , otherwise it will be As the new power system harmonic signal, go to step 3 and repeat k times to get ,use value to determine whether each screening result meets the IMF condition:
式中,为对重复次所得的分量,的取值范围通常在0.2~0.3。满足的要求时,则将作为电力系统谐波信号的第一阶IMF分量,记为,将从 In the formula, for right repeat The amount of time obtained, The value range of is usually 0.2~0.3. satisfy When requested, the As the first-order IMF component of the power system harmonic signal, denoted as ,Will from
电力系统谐波信号中分离出来,得到剩余分量: Power system harmonic signal Separated from and get the remaining components:
式中,是分解出第一阶IMF分量之后的剩余分量。 In the formula, is the remaining component after decomposing the first-order IMF component.
步骤7:将作为新的电力系统谐波信号,重复步骤3-6,直到最终剩余分量为一个常量或者是一个单调函数。于是电力系统谐波信号的EMD分解结果可以表示为: Step 7: Put As a new power system harmonic signal , repeat steps 3-6 until the final remaining components be a constant or a monotonic function. So the EMD decomposition result of the power system harmonic signal can be expressed as:
上式中,为电力系统谐波EMD分解完成之后的IMF分量,m为IMF阶数。 In the above formula, is the IMF component after the power system harmonic EMD decomposition is completed, and m is the IMF order.
步骤8:EMD分解完成后,对电力系统谐波进行时频分析。首先,对EMD分解得到的任 Step 8: After the EMD decomposition is completed, time-frequency analysis is performed on the power system harmonics. First, any EMD decomposition obtained
意一阶IMF分量进行Hilbert变换,则: It means that the first-order IMF component is subjected to Hilbert transformation, then:
上式中,是的Hilbert变换。 In the above formula, yes The Hilbert transform.
步骤9:定义的解析信号: Step 9: Define The parsed signal:
式中,即为的解析信号。 In the formula, that is analysis signal.
步骤10:根据解析信号求解IMF分量的瞬时幅值、瞬时相位和瞬时频率: Step 10: Solve for the instantaneous amplitude, instantaneous phase, and instantaneous frequency of the IMF component from the analytical signal:
上式中,、和分别表示瞬时幅值、瞬时相位和瞬时频率。至此,由步骤9-10可以求出任意一阶固有模态函数瞬时功率、瞬时相位和瞬时频率。 In the above formula, , and represent the instantaneous amplitude, instantaneous phase, and instantaneous frequency, respectively. So far, the instantaneous power, instantaneous phase and instantaneous frequency of any first-order intrinsic mode function can be obtained from steps 9-10.
步骤11:求出瞬时功率、瞬时相位和瞬时频率之后,继续求解Hilbert谱,省略剩余分量,并定义Hilbert谱,记作: Step 11: After calculating the instantaneous power, instantaneous phase and instantaneous frequency, continue to solve the Hilbert spectrum, omitting the remaining components , and define the Hilbert spectrum, denoted as:
上式中,。 In the above formula, .
步骤12:进一步求解Hilbert边际谱,记作: Step 12: Further solve the Hilbert marginal spectrum, denoted as:
Hilbert边际谱提供了每一个频率值上分布的总的振幅和能量,它以概率的形式表示在整个数据序列上的累计振幅或能量,至此,利用改进EMD端点效应的HHT对电力系统谐波信号完成检测分析。 The Hilbert marginal spectrum provides the total amplitude and energy distributed on each frequency value, which expresses the cumulative amplitude or energy on the entire data sequence in the form of probability. So far, the HHT of the improved EMD endpoint effect is used for the harmonic signal of the power system Complete assay analysis.
附图2-11为利用改进前和改进后的镜像法进行仿真得到效果图:其中,图2是镜像法进行改进之前的信号包络效果图和原始信号与上下包络线均值之差的效果图,图3是镜像法进行改进之前对电力系统谐波进行EMD分解的效果图,图4是镜像法进行改进之前对电力系统谐波求得的瞬时频率和瞬时幅值,图5是镜像法进行改进之前对电力系统谐波求解得到的Hilbert谱,图6是镜像法进行改进之前对电力系统谐波求解得到的Hilbert边际谱,图7是镜像法进行改进之后的信号包络效果图和原始信号与上下包络线均值之差的效果图,图8是镜像法进行改进之后对电力系统谐波进行EMD分解的效果图,图9是镜像法进行改进之后对电力系统谐波求得的瞬时频率和瞬时幅值,图10是镜像法进行改进之后对电力系统谐波求解得到的Hilbert谱,图11是镜像法进行改进之后对电力系统谐波求解得到的Hilbert边际谱。 Accompanying drawing 2-11 is the effect diagram obtained by simulation using the mirror method before and after improvement: Among them, Fig. 2 is the effect diagram of the signal envelope before the mirror method is improved and the effect of the difference between the original signal and the mean value of the upper and lower envelopes Fig. 3 is the effect diagram of EMD decomposition of power system harmonics before the mirror method is improved, Fig. 4 is the instantaneous frequency and instantaneous amplitude of the power system harmonics before the mirror method is improved, and Fig. 5 is the mirror image method The Hilbert spectrum obtained by solving the harmonics of the power system before the improvement is made. Figure 6 is the Hilbert marginal spectrum obtained by solving the harmonics of the power system before the improvement of the mirror method. Figure 7 is the signal envelope after the mirror method is improved and the original The effect diagram of the difference between the signal and the mean value of the upper and lower envelopes. Figure 8 is the effect diagram of the EMD decomposition of the power system harmonics after the mirror method is improved. Figure 9 is the instantaneous power system harmonics obtained after the mirror method is improved. Frequency and instantaneous amplitude, Figure 10 is the Hilbert spectrum obtained by solving the power system harmonics after the mirror method is improved, and Figure 11 is the Hilbert marginal spectrum obtained by solving the power system harmonics after the mirror method is improved.
以上是本发明的较佳实施例,凡依本发明技术方案所作的改变,所产生的功能作用未超出本发明技术方案的范围时,均属于本发明的保护范围。 The above are the preferred embodiments of the present invention, and all changes made according to the technical solution of the present invention, when the functional effect produced does not exceed the scope of the technical solution of the present invention, all belong to the protection scope of the present invention. the
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Application publication date: 20140723 |