Abstract

Dynamics of high beta toroidal pinch plasmas in the major radius plane are calculated after a simple model and compared with experimental results of STP-2 screw pinch1) which is operated under the condition of Te≃20 eV and ne≃1.2×1015/cm3. It is demonstrated that the calculation agrees with the experimental results in the early phase of the discharge where the plasma keeps a high beta value (poloidal βp≃3) while the discrepancy between them begins to grow after 8 µs from the start of the main discharge because the βp value decreases considerably. In order not to deviate the plasma column from the center of the discharge tube a concept of the effective dissipative force generated by a proper programming of the pulsed vertical field is introduced. It is demonstrated that this concept is useful to keep the shock-heated high beta plasma in the center of the discharge tube since unfavorable toroidal expansion disappears completely in a few microseconds by a proper programming of the pulsed vertical field.

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