Temporary overvoltage identification method for a power distribution network
An identification method and overvoltage technology, applied in the measurement of current/voltage, measurement of electrical variables, measurement devices, etc., can solve the problems of low discrimination, poor applicability, only applicable, etc., and achieve low feature dimension and strong noise immunity. , the effect of strong applicability
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Embodiment 1
[0040] Example Figure 1-2 As shown, a distribution network temporary overvoltage identification method includes the following steps:
[0041] S1: Obtain and record the three-phase voltage waveform of the bus three-phase power supply in real time;
[0042] S2: extract the zero-sequence voltage within 4 continuous periodic waves after the overvoltage occurs;
[0043] S3: Input the zero-sequence voltage as the signal to be measured into the atomic decomposition algorithm to iteratively find the atomic parameters of the optimal atom that best matches the signal to be measured γ=(f, ρ, φ, t s ,t e ), the signal to be tested is subtracted from the optimal atom to obtain the residual signal, and the relative matching degree P i , where f is the frequency, ρ is the attenuation coefficient; φ is the phase, t s is the starting time, t e is the end time;
[0044] S4: Divide the optimal atoms into the corresponding frequency bands according to the frequency, and calculate the atomi...
Embodiment 2
[0057] Example Figure 1-2 As shown, a distribution network temporary overvoltage identification method includes the following steps:
[0058] S1: Obtain and record the three-phase voltage waveform of the bus three-phase power supply in real time;
[0059] S2: Extract the zero-sequence voltage within four continuous periodic waves after the overvoltage occurs;
[0060] S3: Input the zero-sequence voltage as the signal to be measured into the atomic decomposition algorithm to iteratively find the atomic parameters of the atom that best matches the signal to be measured γ=(f, ρ, φ, t s ,t e ), where f is the frequency, ρ is the attenuation coefficient; φ is the phase, t s and t e Respectively start and end time;
[0061] S4: Calculate the atomic energy E for each frequency band i , and then the atomic energy E of each frequency band i Splicing to obtain the atomic energy array E of the waveform, the frequency band is the bandwidth of the signal to be measured;
[0062] S...
Embodiment 3
[0090] The simulated waveforms are derived from such as image 3 The ATP-EMTP simulation model shown is built based on the primary main wiring and basic data of a substation. Among them, T1 is the 110 / 10kV main transformer, T2 is the 10 / 0.4kV distribution transformer, and the 10kV side is the neutral point ungrounded system; the numbers starting with "F" are the failure points set by the simulation experiment; the load is determined by (20 +j40) equivalent replacement; there is an electromagnetic voltage transformer on the bus; K1 is a time-controlled switch, and Rf is a transition resistance, which is used to simulate a ground fault; the feeder has a total of all overhead (OL) lines, all cable (CL) lines and There are three types of wire-cable hybrid lines, and the line parameters are the same as those in [8]. The simulation sampling rate is taken as 10kHz.
[0091] use image 3 The simulation model shown generates five types of temporary overvoltage waveforms as a sample ...
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