高电压技术
高電壓技術
고전압기술
HIGH VOLTAGE ENGINEERING
2012年
8期
2137-2144
,共8页
邓军波%松岗成居%熊田亚纪子%日高邦彦%蒲路%张冠军
鄧軍波%鬆崗成居%熊田亞紀子%日高邦彥%蒲路%張冠軍
산군파%송강성거%웅전아기자%일고방언%포로%장관군
残余电荷%沿面放电%电荷积聚%高速相机%记忆效应%冲击电压
殘餘電荷%沿麵放電%電荷積聚%高速相機%記憶效應%遲擊電壓
잔여전하%연면방전%전하적취%고속상궤%기억효응%충격전압
residual charge%surface discharge%charge accumulation%high speed camera%memory effects%impulse voltage
固体绝缘的表面是高压电力设备绝缘的最薄弱环节,很多绝缘事故都是由沿面放电造成的。发生放电后,电荷会在绝缘表面积聚,会很大程度上影响下一次放电的产生与发展。为此,通过观测在极性交替变化的冲击电压作用下沿同轴圆柱形聚对苯二甲酸乙二醇酯(PET)绝缘表面放电的发展以及测量放电后表面残余电荷电位的分布,来研究残余电荷对沿面放电的影响。研究表明,在改变冲击电压的极性后,由于反极性残余电荷的影响,放电会被促进,放电通道会沿着前一次放电的通道向前发展,并且会比前一次放电距离略长,放电的强度会增强,放电的发展速度也会加快。在沿着放电通道方向,表面电荷电位梯度可以明显分为两部分:在放电头部的20mm区域,电位梯度较大,为流注放电;而在后面的主干部,电位梯度平缓,为先导放电。
固體絕緣的錶麵是高壓電力設備絕緣的最薄弱環節,很多絕緣事故都是由沿麵放電造成的。髮生放電後,電荷會在絕緣錶麵積聚,會很大程度上影響下一次放電的產生與髮展。為此,通過觀測在極性交替變化的遲擊電壓作用下沿同軸圓柱形聚對苯二甲痠乙二醇酯(PET)絕緣錶麵放電的髮展以及測量放電後錶麵殘餘電荷電位的分佈,來研究殘餘電荷對沿麵放電的影響。研究錶明,在改變遲擊電壓的極性後,由于反極性殘餘電荷的影響,放電會被促進,放電通道會沿著前一次放電的通道嚮前髮展,併且會比前一次放電距離略長,放電的彊度會增彊,放電的髮展速度也會加快。在沿著放電通道方嚮,錶麵電荷電位梯度可以明顯分為兩部分:在放電頭部的20mm區域,電位梯度較大,為流註放電;而在後麵的主榦部,電位梯度平緩,為先導放電。
고체절연적표면시고압전력설비절연적최박약배절,흔다절연사고도시유연면방전조성적。발생방전후,전하회재절연표면적취,회흔대정도상영향하일차방전적산생여발전。위차,통과관측재겁성교체변화적충격전압작용하연동축원주형취대분이갑산을이순지(PET)절연표면방전적발전이급측량방전후표면잔여전하전위적분포,래연구잔여전하대연면방전적영향。연구표명,재개변충격전압적겁성후,유우반겁성잔여전하적영향,방전회피촉진,방전통도회연착전일차방전적통도향전발전,병차회비전일차방전거리략장,방전적강도회증강,방전적발전속도야회가쾌。재연착방전통도방향,표면전하전위제도가이명현분위량부분:재방전두부적20mm구역,전위제도교대,위류주방전;이재후면적주간부,전위제도평완,위선도방전。
For a high-voltage electrical apparatus,its surface insulation is always the weakest point,and many accidents are initiated from surface discharge.After the discharge,charges accumulate on the insulator surface,and these residual charges will significantly influence the onset and development of the subsequent discharge.Therefore,we studied surface discharges on the polyethylene terephthalate(PET)film with a coaxial cylindrical configuration by high speed camera under impulse voltages with alternate voltage polarity,and measured the surface potential distribution induced by residual charges after discharges by an electrostatic probe.With the residual charges from surface discharge with opposite polarity,the subsequent discharge propagates by partly following the path of the previous discharge.The discharge current of the surface discharge will be strengthened by the residual charges with the opposite polarity.Along the direction of discharge channel,the surface charge potential distribution can be divided into two parts,i.e.,20 mm area ahead of discharge with bigger potential gradient,to be streamer discharge,and smooth potential gradient area along the main channel of discharge,to be leader discharge.