DEMO-FNS磁场被动还原和中性束流注入器屏蔽方法分析

S. Ananyev, E. Dlougach, A. V. Klishchenko
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摘要

聚变中子源(FNS)的稳态运行需要等离子体加热并通过快速原子束注入维持其中的电流。DEMO-FNS项目假设使用6个注入器,在500 keV的原子能下提供高达30 MW的额外加热功率。作为DEMO-FNS注入器的原型,为ITER项目详细开发的注入器可以使用。注入器的整体布局可以保留,但由于光束能量和功率的差异,需要改变单个组件。在这些元件内部,对磁场大小有非常严格的限制:沿离子运动路径,磁通密度应低于某一值,在中和区更低。为了在高散射场环境中实现这些特性,由于设施的磁系统-包括极向和环向场的线圈,中央螺线管和等离子体本身-需要对注入器进行额外的屏蔽。在这个阶段,我们期望所提出的设计将允许仅使用无源屏蔽获得所需的磁场值。该屏蔽将由具有高磁导率指数的铁磁材料制成的外壳形成。利用ANSYS代码进行了三维建模,对这种筛的有效性进行了电磁分析。此外,利用BTR代码计算了在得到的磁场条件下,考虑再电离的沿整个注入路径长度的功率负荷。
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Analysis of the DEMO-FNS magnetic field passive reduction and neutral beam injectors shielding methods
Steady-state operation of a fusion neutron source (FNS) will require plasma heating and maintaining the current therein by fast atom beam injection. The DEMO-FNS project assumes the use of six injectors providing additional heating power up to 30 MW at an atomic energy of 500 keV. As a prototype for the DEMO-FNS injector, an injector developed in detail for the ITER project can be used. The overall injector layout may be retained, but changes in individual components will be required due to the difference in beam energy and power. Inside these components, there are very strict restrictions on the magnetic field magnitude: the flux density should be below a certain value along the path of ion movement and even lower in the neutralization region. To achieve these characteristics in an environment with a high scattered field due to the magnetic system of the facility – including the coils of the poloidal and toroidal fields, the central solenoid and the plasma itself – additional shielding of the injectors is required. At this stage, we expect that the proposed design will allow obtainment of the required magnetic field values using only passive shielding. The shield would be formed of a case made of ferromagnetic material with a high magnetic permeability index. An electromagnetic analysis of the effectiveness of such a screen was performed using 3D modeling using the ANSYS code. In addition, the BTR code was used to calculate power loads along the entire injection path length in the obtained magnetic fields conditions, taking into account reionization.
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