在电力需求日益增加而能源资源及负荷分布极不均衡的国情下,对特高压输电技术的深入研究和完善刻不容缓,其中特高压输电线路无线电干扰水平的准确评估和控制极为关键.目前特高压交流线路无线电干扰研究方法中使用较普遍的是激发函数法,...在电力需求日益增加而能源资源及负荷分布极不均衡的国情下,对特高压输电技术的深入研究和完善刻不容缓,其中特高压输电线路无线电干扰水平的准确评估和控制极为关键.目前特高压交流线路无线电干扰研究方法中使用较普遍的是激发函数法,该文采用一种更适合我国国情的激发函数对特高压线路无线电干扰进行研究,在2维模型的基础上用考虑弧垂的等效分析法进行了算例仿真,并与已运行的1 000 k V晋东南-南阳-荆门特高压交流示范工程线路无线电干扰实测数据进行对比,发现考虑弧垂的等效分析法更适用于实际工程,说明了实际特高压线路工程无线电干扰预测中考虑弧垂的必要性.最后分析了无线电干扰影响因素并提出了相应的减弱干扰措施,可为国家特高压输电线路以及杆塔的设计选型提供重要参考.展开更多
The laser-induced plasma wakefield in a capillary is investigated on the basis of a simple two-dimensional analytical model. It is shown that as an intense laser pulse reshaped by the capillary wall propagates in capi...The laser-induced plasma wakefield in a capillary is investigated on the basis of a simple two-dimensional analytical model. It is shown that as an intense laser pulse reshaped by the capillary wall propagates in capillary plasma, it resonantly excites a strong wakefield if a suitable laser pulse width and capillary radius are chosen for a certain plasma density. The dependence of the laser width and capillary radius on the plasma density for resonance conditions is considered. The wakefield amplitude and longitudinal scale of bubbles in capillary plasma are much larger than those in unbounded plasma, so the capillary guided plasma wakefield is more favorable to electron acceleration.展开更多
文摘在电力需求日益增加而能源资源及负荷分布极不均衡的国情下,对特高压输电技术的深入研究和完善刻不容缓,其中特高压输电线路无线电干扰水平的准确评估和控制极为关键.目前特高压交流线路无线电干扰研究方法中使用较普遍的是激发函数法,该文采用一种更适合我国国情的激发函数对特高压线路无线电干扰进行研究,在2维模型的基础上用考虑弧垂的等效分析法进行了算例仿真,并与已运行的1 000 k V晋东南-南阳-荆门特高压交流示范工程线路无线电干扰实测数据进行对比,发现考虑弧垂的等效分析法更适用于实际工程,说明了实际特高压线路工程无线电干扰预测中考虑弧垂的必要性.最后分析了无线电干扰影响因素并提出了相应的减弱干扰措施,可为国家特高压输电线路以及杆塔的设计选型提供重要参考.
基金supported by National Natural Science Foundation of China (No.11047152)the Natural Science Foundation of Jiangxi Province of China (No.2010GQW0048)
文摘The laser-induced plasma wakefield in a capillary is investigated on the basis of a simple two-dimensional analytical model. It is shown that as an intense laser pulse reshaped by the capillary wall propagates in capillary plasma, it resonantly excites a strong wakefield if a suitable laser pulse width and capillary radius are chosen for a certain plasma density. The dependence of the laser width and capillary radius on the plasma density for resonance conditions is considered. The wakefield amplitude and longitudinal scale of bubbles in capillary plasma are much larger than those in unbounded plasma, so the capillary guided plasma wakefield is more favorable to electron acceleration.