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A numerical tool to optimize voltage waveforms for plasma breakdown and early ramp-up in the presence of constraints
•A new algorithm to design voltage waveforms for plasma Breakdown in Tokamaks.•Takes into account quadratic constraints as force and power in an efficient way.•Includes switching network resistors an BD time via a Genetic Algorithm approach.•The procedure is proved to be effective on DEMO. Plasma in...
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Published in: | Fusion engineering and design 2022-03, Vol.176, p.113027, Article 113027 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | •A new algorithm to design voltage waveforms for plasma Breakdown in Tokamaks.•Takes into account quadratic constraints as force and power in an efficient way.•Includes switching network resistors an BD time via a Genetic Algorithm approach.•The procedure is proved to be effective on DEMO.
Plasma initiation is an important phase in a tokamak discharge. The main objective of magnetic control in this phase is to first obtain sufficiently high electric field and connection length (implying a low poloidal magnetic field) in the breakdown region, and then, once plasma is formed, to force the plasma current to increase, guaranteeing force balance equilibrium. The problem is dominated by the presence of significant eddy currents induced in the passive structures and by the many constraints due to the coil system and power supplies. The present paper shows how, with minor simplifying hypotheses, the magnetic control design problem can be converted into a Quadratic Programming problem with both linear and quadratic constraints that can be solved with an ad hoc iterative algorithm. On the other hand, the full design problem, including the choice of possible Switching Network resistors, becomes nonlinear and an evolutionary Genetic Algorithm solver is proposed. The algorithms are tested on DEMO breakdown and early ramp-up design which is a quite challenging problem because of the large distance between active coils and vacuum chamber, the presence of shielding passive structures with large time constants, and the active constraints on the CS/PF coil system. |
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ISSN: | 0920-3796 1873-7196 |
DOI: | 10.1016/j.fusengdes.2022.113027 |