A Frequency Domain Method for Fault Location of HVDC Grounding Electrode Line Based on Distributed Parameter Model
A distributed parameter model, high-voltage direct current technology, applied in the direction of fault location, information technology support system, etc., can solve the problems of low voltage level of the ground electrode line, affect the DC bipolar system, and cannot measure distance, etc., and achieve easy implementation and high measurement accuracy High, simple algorithm effect
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Embodiment 1
[0040] Example 1: ±800kV DC ground electrode line such as figure 1 shown. The line parameters are as follows: the total length of the line is 80km, the DC impedance is 0.023165Ω / km, and the pole resistance is 0.2Ω. The data sampling rate is 6.4kHz. Ground electrode line l 2 A ground fault occurs 20km away from the measuring end, and the transition resistance is 20Ω.
[0041] (1) Using Fast Fourier Transform (FFT), Chebyshev window is selected as the window function, the data window length is N=128, and the dominant frequency component of the electrical quantity at the measurement terminal f=600 Hz is extracted. Calculate the voltage electric current The magnitude and phase of , calculate the voltage and current along the line:
[0042]
[0043]
[0044] (2) Voltage electric current Calculate pole voltage and current
[0045]
[0046]
[0047] (3) Utilize pole address point parameters and line l 1 electric current deduced line l 2 current
[00...
Embodiment 2
[0058] Example 2: ±800kV DC ground electrode line such as figure 1 shown. The line parameters are as follows: the total length of the line is 80km, the DC impedance is 0.023165Ω / km, and the pole resistance is 0.2Ω. The data sampling rate is 6.4kHz. Ground electrode line l 2 A ground fault occurs 40km away from the measuring end, and the transition resistance is 4Ω.
[0059] (1) Using Fast Fourier Transform (FFT), Chebyshev window is selected as the window function, the data window length is N=128, and the dominant frequency component of the electrical quantity at the measurement terminal f=600 Hz is extracted. Calculate the voltage electric current magnitude and phase, calculate the voltage and current along the
[0060]
[0061]
[0062] (2) Voltage electric current Calculate pole voltage and current
[0063]
[0064]
[0065] (3) Utilize pole address point parameters and line l 1 electric current deduced line l 2 current
[0066]
[0067]...
Embodiment 3
[0076] Example 3: ±800kV DC ground electrode line such as figure 1 shown. The line parameters are as follows: the total length of the line is 80km, the DC impedance is 0.023165Ω / km, and the pole resistance is 0.2Ω. The data sampling rate is 6.4kHz. Ground electrode line l 2 A ground fault occurs 70km away from the measuring end, and the transition resistance is 4Ω.
[0077] (1) Using Fast Fourier Transform (FFT), Chebyshev window is selected as the window function, the data window length is N=128, and the dominant frequency component of the electrical quantity at the measurement terminal f=600 Hz is extracted. Calculate the voltage electric current magnitude and phase, calculate the voltage and current along the
[0078]
[0079]
[0080] (2) Voltage electric current Calculate pole voltage and current
[0081]
[0082]
[0083] (3) Utilize pole address point parameters and line l 1 electric current deduced line l 2 current
[0084]
[0085]...
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