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束流

束流的相关文献在1954年到2023年内共计1286篇,主要集中在原子能技术、无线电电子学、电信技术、物理学 等领域,其中期刊论文198篇、会议论文28篇、专利文献164898篇;相关期刊77种,包括中国科学技术大学学报、中国科学院院刊、医疗卫生装备等; 相关会议15种,包括中国核学会2011年年会、2007军工精密与特种加工技术交流会、第七届全国医用加速器学术交流会等;束流的相关文献由2300位作者贡献,包括宋云涛、张天爵、安世忠等。

束流—发文量

期刊论文>

论文:198 占比:0.12%

会议论文>

论文:28 占比:0.02%

专利文献>

论文:164898 占比:99.86%

总计:165124篇

束流—发文趋势图

束流

-研究学者

  • 宋云涛
  • 张天爵
  • 安世忠
  • 丁开忠
  • 管锋平
  • 宋国芳
  • 陈永华
  • 吕银龙
  • 李君君
  • 李明
  • 期刊论文
  • 会议论文
  • 专利文献

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    • 周宏敏; 付圣权; 李明; 黄健柳
    • 摘要: 扫描电镜为材料形貌和成分分析中普遍使用的仪器,但部分材料由于导电性及导热性差,在实际观测过程中容易发生形貌变形。本实验以蓝绿藻、有机高分子和金属有机框架材料为样品,研究了不同加速电压和束流条件下对观测样品形貌的影响。实验结果表明对于热敏感材料,电子束总能量在一定范围内时,与束流相比,加速电压对材料的影响更大,优先采用降低加速电压更合适。
    • 庹还湘; 孙葆根; 罗箐; 吴芳芳; 周天雨; 卢平
    • 摘要: 单谐振腔束团长度监测器利用谐振腔内的两个本征模式测量ps量级的电子束团长度,它的关键是如何将两个不同频率的模式互不干扰地耦合提取出来。为解决这个问题,基于低通和带通滤波器的理论,提出了同轴滤波耦合结构和膜片加载波导滤波结构,借助CST微波工作室对滤波器进行建模并仿真得到其S参数。为测试耦合器的应用效果,设计了一套带有该耦合结构的单谐振腔束团长度监测器探头,根据国家同步辐射实验室基于可调谐红外激光的能源化学研究大型实验装置FELiChEM的束流特点,在CST内对所设计的探头进行束流模拟仿真。仿真结果表明,该耦合器可以实现对特定模式的耦合,并有效降低其它模式的干扰,采用同轴滤波耦合结构和膜片加载波导滤波结构的谐振腔监测器可以实现对FELiChEM装置束团长度的高精度测量,测量误差小于2%。
    • 鲍士伟
    • 摘要: 测试联作施工中,下放管柱过程中一直存在水锤,然而墩钻产生的水锤是能够将起爆器砸响的.研制一款装置保护起爆器抗击水锤,从根本上杜绝施工过程中起爆器提前起爆现象.
    • 孙明明; 耿海; 杨俊泰; 岳士超; 张文涛
    • 摘要: 为了研究30 cm离子推力器束流引出状态对栅极刻蚀的影响,建立了束流引出模型,并采用PIC-MCC方法对CEX离子造成的栅极腐蚀速率进行了计算,最后将计算结果与1500 h寿命试验结果进行比对分析.结果显示:束流正常聚焦时,在3 kW和5 kW两种工作模式下,加速栅和减速栅的质量刻蚀速率分别为(1.11~1.72)×10?15 kg/s及(1.22~1.26)×10?17 kg/s.在5 kW工况下,当屏栅上游等离子体密度达到4.03×1017 m?3时,束流出现欠聚焦现象,此时加速栅和减速栅的最大离子刻蚀速率分别为4.33×10?15 kg/s和4.02×10?15 kg/s;在3 kW工况下,当屏栅上游等离子体密度达到0.22×1017 m?3时,束流出现过聚焦现象,此时加速栅和减速栅的最大离子刻蚀速率分别为3.24×10?15 kg/s和5.01×10?15 kg/s.寿命试验结果表明,加速栅孔质量刻蚀速率的计算值与试验值比对误差较小,而由于束流离子对减速栅孔的直接轰击,导致减速栅孔刻蚀速率的计算值和试验值差异极大.经研究认为,对屏栅小孔采用变孔径设计,是降低当束流处于欠聚焦或过聚焦状态下,CEX离子造成加速栅孔和减速栅孔刻蚀速率,并提升推力器工作寿命的有效措施.
    • 阚朝新; 胡跃明; 包轶文; 范宏盛
    • 摘要: 2020年HI-13串列加速器运行正常。全年加速器开机运行3500h,为近40个用户提供了3050h的束流时间,提供的离子种类19种。供束时间按离子分配如图1所示。加速器头部电压运行范围3~12 MV。
    • 赵木; 常晟; 尚自强
    • 摘要: 介绍了质子治疗的特点和其治疗过程及不同设备的技术特点,分析了加速器、束流传输系统、治疗舱等主工艺设备选择的各种影响因素及质子治疗中心建筑功能设计要求,指出了主工艺设备的选型、布置与质子治疗中心建筑方案、功能要求的关系,并展望了质子治疗设备的未来应用前景.
    • 许海鹰; 桑兴华; 邢一思; 左从进; 崔向中; 姜春竹
    • 摘要: 为了提高EB-PVD设备性能、增强其工作灵活性,基于三级AC-DC拓扑电路、多路逆变电路串并联技术、双闭环控制策略分别设计制造了加速电源、灯丝加热电源,并将所研制加速电源、灯丝加热电源与两极电子枪、真空系统、控制系统等进行集成,组成EB-PVD试验装置,分别测试了该装置输出的高压、最大束流、灯丝加热电流、功率变压器输入波形等.试验结果表明:所研制的逆变电源输出高压达到-30kV,束流输出时逆变电源输出特性为恒压特性;灯丝加热电流最大150A,最大束流达到2000mA.这表明所研制的逆变电源满足EB-PVD设备工作需求.%In order to enhance the performance and flexibility of EB-PVD machine, the topology circuit of three parts of AC-DC circuits, the technology of several circuits in series and parallel connection, and double closed loop control have been adopted to design high voltage power supply and filament heating power supply. The inverter power supply, fila-ment heating power supply, EB-PVD gun, vacuum system and others control system were assembled to establish a set of EB-PVD test equipment. Besides the high voltage and the maximal EB current output have been detected, the current of filament heating power supply and the input waves of power transformers also have been measured. Through the series of tests, the results show that not only the maximum high voltage output is up to -30kV, but also the inverter power supply has a good constant voltage character during electron beam output. The maximum electron beam current is up to 2000mA at 150A filament heating current. These test results show that the inverter power supply has fine applicability for EB-PVD machine.
    • 龙建飞; 张天平; 杨威; 孙明明; 贾艳辉; 刘明正
    • 摘要: 离子推力器推力密度分布对航天器轨道维持和修正具有重要影响.采用粒子模拟-蒙特卡罗碰撞方法模拟束流等离子体输运过程,分析束流多组分粒子喷出数量和速度等微观参数,并计算得到单孔束流推力,结合放电室出口等离子体密度分布,进一步对推力密度分布特性分析,最后开展实验验证.研究结果显示:束流中单价离子、双荷离子以及交换电荷离子的推力贡献比分别为84.63%, 15.35% 和1.82%,可见推力主要来源于束流中的单价离子和双荷离子,交换电荷离子对推力贡献很小;推力密度分布具有较好的中心轴对称性,从推力器中心沿着径向先快速下降后趋于缓慢;与实验结果对比,经验模型相对误差约为4.1%,数值模型相对误差约为2.8%,相比经验模型,数值模型具有更好的准确性.研究结果可为离子推力器推力密度分布均匀性等优化提供参考.%Thrust density distribution of ion thruster is an important factor that affects the orbit correction and station keeping of the spacecraft. Current empirical models mainly concern themselves with the overall thrust of the ion thruster, yet the thrust density distribution has not been fully understood. Hence it is necessary to investigate the thrust density characteristics of the ion thruster to devise the approach to optimizing the thruster performances. In this study, the thrust density characteristics of the ion thruster is analyzed and discussed by combining the empirical and theoretical methods. An ion thruster utilizes biased grids to extract ions from discharge chamber and accelerate them to high velocities, thereby forming a beam and generating thrust. In this paper, we analyze the working process of the ion thruster. The thrust expression as a function of beam micro-particle parameters is presented. Meanwhile the transport process of the plasma in the beam stream is simulated by the particle in cell-Monte Carlo (PIC-MCC) method for two-grid optics. The motion behavior of ions is modeled by the PIC method,while the collisions of particles are modeled by the MCC method. In the simulation, the particle trajectories are traced and the micro information about ejected charged ions is recorded with respect to singly charged ion, doubly charged ion and charge exchanged (CEX) ion. By analyzing the density and axial velocity of the charged particles in the beam stream,the thrust of the beam from a single grid hole can be calculated, based on which the thrust distribution of the thruster can be inferred by considering the distribution of plasma density at the exit of discharge chamber. Moreover, the above theoretical analysis of the thrust density is tested experimentally. The studies show that the thrust contribution percentages of the singly charged ion, doubly charged ion and CEX ion in the beam current are 84.63%, 15.35%, and 1.82%, respectively. Apparently, the main contributions to the thrust are made by the singly charged ions and doubly charged ions in the beam plasma,while the CEX ions have a trivial effect on the variation of the thrust. The distribution of the thrust density shows good symmetry along the central axis and it levels off after a fast decline in the radial direction. Comparisons of empirical and numerical results with the experimental results show that the empirical results have an error of about 4.1% and the numerical results have an error of about 2.8%. This indicates that the computational accuracy of our numerical model is better than that of the empirical model This work provides a reference for optimizing the thrust density uniformity of an ion thruster.
    • 张立锋; 杨圣; 刘保杰; 余国龙; 韩广文; 朱志斌
    • 摘要: 本文介绍了一种应用于多能量档电子直线加速器栅控电子枪的专用电源.根据栅控电子枪的工作需求,电子枪的阴极处于-50 kV高压上,电源的3路输出,包括灯丝电源、偏压电源和栅控脉冲电源,均通过高压隔离变压器,将信号输送到高压端的灯丝、阴极和栅极上.利用主控计算机精确调节了电子枪发射束流的大小和脉冲宽度,以满足加速器多能量输出的需求.高压端均为无源器件,以降低故障率.此电源结构简单、调节方便、工作稳定,已在多能量档电子直线加速器上连续工作近4 a,运行状态良好.
    • 摘要: 9月1日,位于广东东莞的国家大科学装置——中国散裂中子源(CSNS)科研团队召开新闻发布会,宣布中国散裂中子源于8月28日首次打靶成功,获得中子束流。这标志着散裂中子源主体工程顺利完工,进入试运行阶段。
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