Device and method for measuring surface charge distribution of basin-type insulator before and after surface flashover
A technology of basin-type insulators and surface flashover, which is applied to measuring devices, measuring electricity, measuring electrical variables, etc., can solve the problem of difficult to measure the surface charge before and after flashover, and achieves the saving of measuring time, the method is simple and reliable, and the operation is easy. Effect
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Embodiment 1
[0080] Step 1: Wipe the surface of the two pot insulators with a diameter of 180mm to be measured with absolute ethanol, and let it stand for more than 12 hours. The flashover voltage obtained by the 180mm pot insulator is roughly 360kV-420kV, and the 600kV high-voltage DC source can make it flashover along the surface, and then the surface charge distribution before and after the flashover along the surface can be measured.
[0081] Step 2: Install the two pot insulators to be measured in parallel in the 220kV GIS cavity 3, and install shielding covers before and after the pot insulators to shield the high-voltage electrodes, the field strength at the three junctions of the insulator and sulfur hexafluoride gas , connect the surface charge measurement device 6 with the GIS cavity 3, avoid metal debris falling into the GIS cavity 3 during the installation process, connect the high-voltage DC source 1 to the current-limiting resistor 2 through the high-voltage lead, and the curr...
Embodiment 2
[0088] The difference from Example 1 is that the high-voltage DC voltage applied in step 4 is not evenly boosted until the insulator flashover occurs, but is evenly boosted to 400kV at a boosting speed of 5kV / s and then no longer boosted. And keep the DC voltage at 400kV, and wait for the surface flashover of the pot insulator. After the surface flashover occurs, continue the steps of the second embodiment to measure the surface charge distribution of the pot insulator before and after the surface flashover under the long-term withstand voltage.
Embodiment 3
[0090] The difference from the first embodiment is that the high voltage AC voltage is applied in the fourth step.
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