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    • 4. 发明申请
    • NUCLEAR FUSION MACHINE FOR RELEASING ENERGY WITH FEWER NEUTRONS AND WITH AVERAGE FUSION REACTANT ENERGIES GREATER THAN 30 KEV
    • 核聚变机对能源的核聚变反应PARTNER大于30 KEV中间中子武器能量释放
    • WO00067535A1
    • 2000-11-09
    • PCT/DE2000/001351
    • 2000-04-28
    • G21B1/11H05H1/12H05H1/18G21B1/00
    • H05H1/18G21B1/11H05H1/12Y02E30/122Y02E30/124Y02E30/126
    • The relativistic resonance loss that occurs in electron-cyclotron resonance heating (ECRH) of electrons to considerable energies is compensated with frequency comb (FC) ECRH. It is then possible to satisfy the resonance requirement in one place, up to a maximum energy. The considerable average electron energy that can be achieved in this way reduces the Coulomb collision probability and therefore the loss of electrons from the magnetic containment. Any electrons that still escape are reflected back into the magnetic containment by electric fields. The resulting electron energy density reduces the neutral particle density and therefore the collision neutralisation, fully ionising ions so that the charge exchange collisions no longer occur. Appropriate measures are taken to reduce neutron production. The energy of the nuclear fusion reaction products is partially converted directly into electric current. This FCECRH technology can be used in any magnetic field structures. The invention provides a magnetic field structure in which FCECRH technology can used very advantageously for controlled nuclear fusion. FCECRH can also be used to produce a closed, diamagnetic minimum magnetic field channel in which the fusion partners are contained, in tokamaks and stellarators. Further measures can be taken to deepen this channel.
    • 在电子的大的能量的电子回旋共振加热(EZRH)发生的相对论共振损失,(FK)-EZRH与频率梳,其中谐振条件是最多能量补偿满足同一个地方。 可实现的大的平均电子能量减少了他们的库仑碰撞概率,因此电子从磁约束的损失。 尽管如此逸出电子被反射回来通过在磁约束电场。 所产生的电子的能量密度降低Neutralteilchendichte并且因此影响中和。 他们完全电离的离子,使电荷交换颠簸消失。 适当的措施,以减少中子产生。 核聚变反应产物的能量部分被直接转换成电能。 所述FKEZRH技术可以在任何磁场结构被采用。 提出了一种磁场结构,其中FKEZRH技术可非常有利地用于受控核聚变。 具有封闭反磁性最小磁场通道FKEZRH也可以在托卡马克和仿星器生成,其中,所述融合配偶体将被包括在内。 这可以通过进一步的措施来加深。
    • 7. 发明申请
    • PLASMA CONFINEMENT SYSTEMS AND METHODS FOR USE
    • 等离子体约束系统和使用方法
    • WO2017070094A1
    • 2017-04-27
    • PCT/US2016/057494
    • 2016-10-18
    • UNIVERSITY OF WASHINGTON
    • JARBOE, Thomas, R.ROGERS, John, A.
    • H05H1/12H05H1/02
    • H05H1/12G21B1/05H05H1/16Y02E30/122Y02E30/126
    • In one example, a plasma confinement system includes a substantially torus-shaped outer manifold aligned on a mid-plane of the plasma confinement system. The outer manifold includes a first helicity injection port at an inner radius of the outer manifold. The plasma confinement system further includes a substantially torus-shaped inner manifold aligned on the mid-plane within the inner radius of the outer manifold. The inner manifold includes a second helicity injection port at an outer radius of the inner manifold. The plasma confinement system further includes a helicity injection tube on the mid-plane. The helicity injection tube connects the first helicity injection port to the second helicity injection port. Methods for using the plasma confinement system are also disclosed herein.
    • 在一个示例中,等离子体约束系统包括在等离子体约束系统的中平面上对齐的基本上圆环形的外歧管。 外歧管包括在外歧管的内径处的第一螺旋性注射口。 等离子体约束系统还包括在外歧管的内半径内在中平面上对齐的基本上圆环形的内歧管。 内部歧管包括在内部歧管的外半径处的第二螺旋性注入口。 等离子体约束系统还包括在中平面上的螺旋性注入管。 螺旋度注入管将第一螺旋性注入口连接到第二螺旋性注入口。 本文还公开了使用等离子体约束系统的方法。