Abstract
Research & Development in Material Science The Rotating Magnetic Field for Confining and Heating Plasma Vladimir Kuzmich Shilov*, Alexander Nikolaevich Filatov and Alexander Evgenievich Novozhilov National Research Nuclear University, Russia *Corresponding author: Vladimir Kuzmich Shilov, National Research Nuclear University MEPhI, 31, Kashirskoye shosse, Moscow, 115409, Russian Federation, Russia Submission: February 22, 2018; Published: March 22, 2018 DOI: 10.31031/RDMS.2018.04.000592 Volume 4 Issue 4 March 2018
Highlights
To retain and simultaneously heat the high-temperature plasma, it is proposed to use a magnetic trap creating a closed
Let’s see how the solenoids of the traps placed in three magnetic fields from nine open traps placed in triads in three orthogonal planes are to be phased, in order to obtain a closed orthogonal planes
If we consider that the only way to effectively confine plasma magnetic field, the total magnetic induction vector of which rotates continuously in all three dimensions
Summary
Vladimir Kuzmich Shilov*, Alexander Nikolaevich Filatov and Alexander Evgenievich Novozhilov. In the X-Y plane, projections of the total vector of the magnetic induction on the X and Y axes will be: in a certain volume configuration, it is is the magnetic field proposed to create of a a trap of reactor baapseadrtiocunlaar= Bx1 (t ). Coplanar traps are placed on a circle with a common center, each at 120 degrees to the other Coils of these nine traps lie in a sort of spherical surface and due to overlapping of the magnetic fields create in its center the total magnetic field with a constant magnetic induction vector, which where φ1, φ2, φ3 are initial phases of total vectors of magnetic induction in the planes in question. In the Z-X plane, change of α(t) along the Z-axis (in the direction of the X axis) is equal to: rotates with the frequency of the three-phase current supplied to the coil. Copyright © All rights are reserved by Vladimir Kuzmich Shilov
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