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AC partial discharge characteristic at minute air gap under non-uniform electric field

机译:不均匀电场下微小气隙处的交流局部放电特性

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For a raise of the miniaturization and reliability of various electric power apparatuses, it is important to clarify the partial discharge characteristic in their insulation part. In many case, partial discharge may occur under the non-uniform field. So, it is necessary to understand the partial discharge characteristic under non-uniform electric filed. Partial discharge inception voltage (PDIV) was measured under AC voltage application using needle-plane electrode system. Partial discharge inception electric field (PDIE) was estimated using COMSOL that is a general purpose physical simulation software. When the air gap distance was below 50 μm and the tip radius was 10, 30 and 60 μm, PDIE at the needle tip was almost the same as the electric field estimated by the Paschen curve. In this case, it is considered that PDIV may be decided by the electric field at the needle tip and that the emission of initial electrons plays very important role in the partial discharge process. However, when the needle tip radius was 10 or 30 μm and the air gap distance became 50 μm, PDIE at the needle tip became higher than the electric field strength estimated by the Paschen curve. In this latter case, it is considered that even if initial electron was emitted from the needle tip, the electric field was not enough to develop the detectable electron avalanche. From our experiment, the electric field strength necessary to the detectable partial discharge development is estimated to be about 67 % of the electric field strength necessary to the initial electron emission from the needle tip.
机译:为了提高各种电力设备的小型化和可靠性,重要的是弄清它们的绝缘部分中的局部放电特性。在许多情况下,在非均匀电场下可能会发生局部放电。因此,有必要了解电场不均匀下的局部放电特性。使用针面电极系统在交流电压施加下测量局部放电起始电压(PDIV)。使用通用物理模拟软件COMSOL估算了局部放电起始电场(PDIE)。当气隙距离小于50μm且尖端半径为10、30和60μm时,针尖处的PDIE几乎与通过Paschen曲线估计的电场相同。在这种情况下,认为PDIV可以由针尖处的电场决定,并且初始电子的发射在局部放电过程中起着非常重要的作用。然而,当针尖半径为10或30μm并且气隙距离变为50μm时,针尖处的PDIE变得高于通过帕申曲线估计的电场强度。在后一种情况下,认为即使从针尖发射了初始电子,电场也不足以产生可检测的电子雪崩。根据我们的实验,可检测到的局部放电发展所需的电场强度估计约为从针尖发出初始电子所需的电场强度的67%。

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