高电压技术
高電壓技術
고전압기술
HIGH VOLTAGE ENGINEERING
2012年
5期
1090-1098
,共9页
章程%邵涛%许家雨%马浩%严萍
章程%邵濤%許傢雨%馬浩%嚴萍
장정%소도%허가우%마호%엄평
ns脉冲%脉冲重复频率%极不均匀电场%弥散放电%放电特性%脉冲参数%极性效应
ns脈遲%脈遲重複頻率%極不均勻電場%瀰散放電%放電特性%脈遲參數%極性效應
ns맥충%맥충중복빈솔%겁불균균전장%미산방전%방전특성%맥충삼수%겁성효응
nanosecond-pulse%pulse repetition frequency%inhomogeneous electrical field%diffuse discharge%discharge characteristics%pulse parameters%polarity effect
为了能够在大气压下获得大面积高能量密度的低温等离子体,近年来弥散放电的研究与应用受到广泛关注。采用基于磁脉冲压缩系统的重复频率ns脉冲电源来激励大气压空气中尖板电极结构放电,通过电压电流测量和发光图像拍摄研究了弥散放电的特性。实验结果表明,在常温常压和高重复频率下能够获得大面积均匀的弥散放电,气隙距离增大或减小时,弥散放电分别向电晕放电与火花放电转换。重频ns脉冲放电存在极性效应,电极的小曲率半径处施加负脉冲时需要比正脉冲更高的电场强度才能获得弥散放电。此外,弥散放电的强度随着脉冲上升时间的增大而减弱。因此合适的气隙距离、极不均匀电场的强场处施加正极性脉冲和较陡的脉冲上升时间有利于获得较为强烈的弥散放电。
為瞭能夠在大氣壓下穫得大麵積高能量密度的低溫等離子體,近年來瀰散放電的研究與應用受到廣汎關註。採用基于磁脈遲壓縮繫統的重複頻率ns脈遲電源來激勵大氣壓空氣中尖闆電極結構放電,通過電壓電流測量和髮光圖像拍攝研究瞭瀰散放電的特性。實驗結果錶明,在常溫常壓和高重複頻率下能夠穫得大麵積均勻的瀰散放電,氣隙距離增大或減小時,瀰散放電分彆嚮電暈放電與火花放電轉換。重頻ns脈遲放電存在極性效應,電極的小麯率半徑處施加負脈遲時需要比正脈遲更高的電場彊度纔能穫得瀰散放電。此外,瀰散放電的彊度隨著脈遲上升時間的增大而減弱。因此閤適的氣隙距離、極不均勻電場的彊場處施加正極性脈遲和較陡的脈遲上升時間有利于穫得較為彊烈的瀰散放電。
위료능구재대기압하획득대면적고능량밀도적저온등리자체,근년래미산방전적연구여응용수도엄범관주。채용기우자맥충압축계통적중복빈솔ns맥충전원래격려대기압공기중첨판전겁결구방전,통과전압전류측량화발광도상박섭연구료미산방전적특성。실험결과표명,재상온상압화고중복빈솔하능구획득대면적균균적미산방전,기극거리증대혹감소시,미산방전분별향전훈방전여화화방전전환。중빈ns맥충방전존재겁성효응,전겁적소곡솔반경처시가부맥충시수요비정맥충경고적전장강도재능획득미산방전。차외,미산방전적강도수착맥충상승시간적증대이감약。인차합괄적기극거리、겁불균균전장적강장처시가정겁성맥충화교두적맥충상승시간유리우획득교위강렬적미산방전。
Nanosecond-pulse can generate extremely high power density and large-scale non-thermal plasma, which attracts attentions. We used a repetitive nanosecond-pulse generator based on magnetic compression system to drive gas discharge in atmospheric air with a tube-to-plane gap, and investigated characteristics of diffuse discharge by the measurement of electrical discharge parameters and discharge images. The experimental results show that large scale diffuse discharge can be obtained at atmospheric pressure with high pulse repetition frequency, and the diffuse discharge will transit to corona or spark mode with increasing or decreasing air gap spacing, respectively. Polarity effect occurs in repetitive nanosecond-pulse discharge, with a negative polarity of the electrode of small curvature radius, diffuse discharge needs more electric field for excitation than that with a positive polarity. In addition, intensity of the diffuse discharge decreases with the increase of the rise-time of pulse. Therefore, the diffuse discharge is likely available under certain conditions of proper air gap, high electric field with positive pulse, and fast rise time.