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    • 4. 发明授权
    • Tokamak plasma heating with intense, pulsed ion beams
    • 具有强烈脉冲离子束的托卡马克等离子体加热
    • US4421713A
    • 1983-12-20
    • US247420
    • 1981-03-25
    • Wallace M. ManheimerNiels K. Winsor
    • Wallace M. ManheimerNiels K. Winsor
    • H05H1/22G21B1/02
    • H05H1/22
    • An intense, space-charge-neutralized, pulsed ion beam is used to heat a metically-confined plasma, such as a tokamak plasma, by injecting the ion beam into the plasma along a trajectory that is generally tangential to the confining magnetic field. The ion beam inductively generates a plasma return current so that no net current is produced. As the ion beam drifts in the plasma, the confining magnetic field is transformed into one which can trap the ion beam at the center of the plasma. Once the ion beam is trapped, the plasma return current is cancelled by transformer action to produce a net current which is carried by the ion beam alone. The beam transfers its energy to the plasma by classical collisions with the electrons and ions of the plasma. Heating of the plasma can be sufficient to produce a breakeven condition or ignition.
    • 通过沿着通常与限制磁场相切的轨迹将离子束注入等离子体,使用强烈的空间电荷中和的脉冲离子束来加热磁性约束等离子体,例如托卡马克等离子体。 离子束感应地产生等离子体回流电流,使得不产生净电流。 当离子束在等离子体中漂移时,限制磁场被转换成能够将离子束捕获在等离子体中心的磁场。 一旦离子束被捕获,等离子体返回电流就被变压器作用所抵消,以产生仅由离子束承载的净电流。 光束通过与等离子体的电子和离子的经典碰撞将其能量传递到等离子体。 等离子体的加热足以产生盈亏平衡条件或点火。
    • 8. 发明授权
    • Quasioptical gyroklystron
    • 夸张陀螺仪
    • US4491765A
    • 1985-01-01
    • US414129
    • 1982-09-02
    • Wallace M. ManheimerEdward OttAnders Bondeson
    • Wallace M. ManheimerEdward OttAnders Bondeson
    • H01J25/02H01J25/00
    • H01J25/025
    • A quasioptical gyroklystron for generating high power quasioptical radiation. A mildly relativistic electron beam gyrating in a static magnetic field is passed through a first open mirror resonator where a small change in the transverse electron energy takes place (either an increase or decrease depending on the relative phase between the electron gyration and the resonator wave fields). This small change than leads to slower (or more rapid) gyration of those electrons that have gained (or lost) energy in the first resonator. The length of the drift region between the first and a second open mirror resonator is adjusted so that rapidly gyrating electrons overtake slowly gyrating ones at the entrance to the second resonator. Thus the particles arrive at the second resonator strongly bunched in gyration phase. The fields in the first resonator are generated by feedback of a small amount of energy from the wave mode in the second resonator with a .pi./2 phase lag so that the beam entering the second resonator is bunched at the right phase angle to lose power efficiently to the fields in the second resonator. The lost power is extracted and guided to a utilization device.
    • 用于产生高功率准激光辐射的准激光陀螺仪。 在静态磁场中轻微相对论的电子束旋转通过第一开放镜谐振器,其中发生横向电子能量的小变化(根据电子回转和谐振器波场之间的相对相位而增加或减小 )。 这种小的变化导致在第一谐振器中获得(或丢失)能量的那些电子的较慢(或更快速)回转。 调整第一和第二开启镜谐振器之间的漂移区域的长度,使得快速旋转的电子在第二谐振器的入口处超过缓慢旋转的电子。 因此,颗粒到达第二共振器,在回转阶段中强力聚束。 第一谐振器中的场通过以π/ 2相位滞后从第二谐振器中的波模式的少量能量的反馈产生,使得进入第二谐振器的光束以正确的相位角聚束以有效地失去功率 到第二谐振器中的场。 丢失的功率被提取并被引导到利用装置。