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正交电场下XLPE/SIR介质界面空间电荷特性 被引量:5
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作者 张宇巍 朱有玉 +3 位作者 王霞 吴锴 傅明利 侯帅 《南方电网技术》 北大核心 2015年第10期52-56,共5页
直流电缆附件绝缘和电缆绝缘的界面同时承受着沿着电缆径向的体电场和沿电缆轴向的界面电场,这两个电场在方向上相互正交,在界面上的分布和集中使得复合绝缘界面的空间电荷特性变得复杂。采用交联聚乙烯(crosslinked polyethylene,XLPE... 直流电缆附件绝缘和电缆绝缘的界面同时承受着沿着电缆径向的体电场和沿电缆轴向的界面电场,这两个电场在方向上相互正交,在界面上的分布和集中使得复合绝缘界面的空间电荷特性变得复杂。采用交联聚乙烯(crosslinked polyethylene,XLPE)和硅橡胶(silicone rubber,SIR)制成双层试样模拟附件结构中的复合绝缘,通过界面贴覆铝箔针-板电极(针电极为正/负)、板-板电极三种电极形式为绝缘界面提供正交电场,运用电声脉冲法(pulse electro-acoustic,PEA)分别测量了体电场、正交电场作用下XLPE/SIR界面空间电荷的分布情况。结果表明,在体电场和界面电场的正交电场作用下,XLPE/SIR界面的空间电荷峰值出现明显变化:试样加压20 min后,界面贴覆针电极为负的针-板电极时,界面电荷峰值随施加电场强度的增加先增大后减小,使XLPE侧电极在较低场强下即发生注入;界面贴覆针电极为正的针-板电极时,界面电荷峰值在电场作用下减小,加剧了SIR侧的正电荷注入;在界面板-板电极作用下,界面电荷峰值变化不大,但仍有所下降。 展开更多
关键词 联聚乙烯/硅橡胶 直流附件 正交电场 界面电荷 电声脉冲(PEA)
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两个正交线性电场中的线性斯塔克效应
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作者 张德林 《黑龙江大学自然科学学报》 CAS 1999年第2期83-85,共3页
本文利用微扰法计算了在两个正交线性电场中的线性斯塔克效应,结果表明,氢原子第一激发态能级的一级修正是非简并的。
关键词 斯塔克效应 简并 微扰法 线性电场
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解除氢原子能级(n=3)的简并 被引量:6
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作者 刘兴业 《大学物理》 北大核心 2001年第8期15-18,共4页
讨论氢原子能级在两个正交线性非均匀电场中的分裂
关键词 氢原子 能级 微扰论 线性电场 一级修 简并
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Correction Scheme for Scheduled Network Loss Rate Applied to UHV Transmission Trading
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作者 Yinya Zhang Shunming Bai Yukun Bao 《Journal of Energy and Power Engineering》 2015年第3期303-309,共7页
The size and allocation method of transmission network loss have major impact on particular users involved with the electricity market trading process, therefore, the accuracy of scheduled network loss rates will be v... The size and allocation method of transmission network loss have major impact on particular users involved with the electricity market trading process, therefore, the accuracy of scheduled network loss rates will be vital to the economic concerns from the stakeholders. In view of the shortcoming of existing loss rate scheme in 1,000 kV demonstration project, three scheduled loss rates applied to the UHV AC (ultra high voltage alternating current) transaction settlement are revised. By taking relationship between loss rate and power into consideration, the new segmented correction scheme greatly reduces the deviation between scheduled loss rates and actual loss rates, and is more accurate, flexible and expansible than the old one. 展开更多
关键词 UHV loss rate transaction settlement curve fitting loss allocation.
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Broadband isolated attosecond pulse generation in a two-color laser field combined with an orthogonally polarized laser pulse 被引量:2
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作者 DU HongChuan WANG XiaoShan HU BiTao 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2012年第1期1-6,共6页
We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction,... We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction, a modulated supercontinuum from 290 to 430 eV is obtainable. By properly adding a second-harmonic control field of the driving pulse in the y direction, the short quantum path is well selected and a smooth supercontinuum from 290 to 440 eV is generated. The bandwidth of the supercontinuum can be controlled by adjusting the electric field of the control pulse in the x direction. When the electric field increases to 0.051 a.u., a smooth supercontinuum from 295 to 520 eV is obtained. Using this method we expect that isolated 63-as attosecond pulses with tunable central wavelengths are straightforwardly obtained.We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction, a modulated supercontinuum from 290 to 430 eV is obtainable. By properly adding a second-harmonic control field of the driving pulse in the y direction, the short quantum path is well selected and a smooth supercontinuum from 290 to 440 eV is generated. The bandwidth of the supercontinuum can be controlled by adjusting the electric field of the control pulse in the x direction. When the electric field increases to 0.051 a.u., a smooth supercontinuum from 295 to 520 eV is obtained. Using this method we expect that isolated 63-as attosecond pulses with tunable central wavelengths are straightforwardly obtained. 展开更多
关键词 HHG SUPERCONTINUUM attosecond pulses
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