Dynamic Modeling and Resilience for Power Distribution
US-2015331063-A1 · Nov 19, 2015 · US
US9651604B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9651604-B2 |
| Application number | US-201414897501-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 23, 2014 |
| Priority date | Nov 21, 2013 |
| Publication date | May 16, 2017 |
| Grant date | May 16, 2017 |
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A grounding grid breakpoint diagnostic method for a transient electromagnetic method, based on a transient electromagnetic detection apparatus. The method comprises: ( 101 ) disposing a test line at a position above a grounding grid to be diagnosed on the ground, and determining coordinates of a detection point; ( 102 ) obtaining information about coordinates of the detection point, and coinciding the center of the transient electromagnetic detection apparatus with the coordinates of the detection point; ( 103 ) performing, by the transient electromagnetic detection apparatus, measurement along the test line point by point, so as to obtain measurement data; ( 104 ) processing, by using diagram forming software, the measurement data to form a longitudinal resistivity cross-section diagram of the detection point according to a preset formula; ( 105 ) determining whether a breakpoint occurs at the detection point according to the longitudinal resistivity cross-section diagram. The method does not depend on a design material of a grounding grid, and can implement non-excavation grounding grid breakpoint diagnosis without outage, thereby reducing economic losses in a diagnosis process.
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What is claimed is: 1. A grounding grid breakpoint diagnostic method, based on a transient electromagnetic detection apparatus including a transmitting system and a receiving system, said transmitting system including a battery pack, a transmitter and a transmitting coil, said receiving system including a receiver and a receiving coil, wherein said transmitting coil has its two ends respectively connected to current output ends of said transmitter, said battery pack has its anode connected to a positive power supply terminal of said transmitter and its cathode connected to a negative power supply terminal of said transmitter, and said receiving coil has its two ends respectively connected to signal acquisition lines of said receiver, characterized in that the method comprises: disposing a test line at a position above a grounding grid to be diagnosed on the ground, and determining coordinates of a detection point; obtaining information about coordinates of the detection point, and coinciding the center of the transient electromagnetic detection apparatus with the coordinates of the detection point; performing, by the transient electromagnetic detection apparatus, measurement along the test line point by point, so as to obtain measurement data; processing, by using diagram forming software, the measurement data to form a longitudinal resistivity cross-section diagram of the detection point according to a preset formula; and determining whether a breakpoint occurs at the detection point according to the longitudinal resistivity cross-section diagram. 2. The method as recited in claim 1 , characterized in that the processing, by using diagram forming software, the measurement data to form a longitudinal resistivity cross-section diagram of the detection point according to a preset formula is particularly: starting the transmitter of the transient electromagnetic detection apparatus to generate bipolar rectangular pulse current and establish a primary pulsed magnetic field; observing and sensing a secondary vortex field using the receiving coil of the transient electromagnetic detection apparatus and converting a secondary voltage signal stored in the receiver of the transient electromagnetic detection apparatus into a magnetic field signal; constructing and calculating a function of transient field parameters f(u) using a formula of a vertical component B z of the secondary field B z = Iμ 2 a [ 3 πμ ⅇ - u 2 + ( 1 - 3 2 u 2 ) erf ( u ) ] , the f ( u ) = 1 u 2 [ 3 u π ⅇ - u 2 + ( u 2 - 3 2 ) erf ( u ) ] - 2 aB z μ I , and calculating apparent resistivity ρ(t), the ρ ( t ) =
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