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1 - Nuclear Sciences and Applications - IAEA

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<strong>IAEA</strong>-CN-50/E-IV-7<br />

NON-INDUCTIVE STARTUP AND<br />

CURRENT RAMP-UP SCENARIO OPTIMIZATION<br />

FOR A TOKAMAK REACTOR<br />

G.V.PEREVERZEV<br />

I.V. Kurchatov Institute of Atomic Energy,<br />

Moscow,<br />

Union of Soviet Socialist Republics<br />

Abstract<br />

NON-INDUCTIVE STARTUP AND CURRENT RAMP-UP SCENARIO OPTIMIZATION FOR A<br />

TOKAMAK REACTOR.<br />

The stages of gas ionization <strong>and</strong> current ramp-up in a non-inductive tokamak are considered. The<br />

main feature of this consideration of the ionization stage is the use of the recently developed theory of<br />

plasma equilibrium in a toroidal system without rotational transform. The transport model based on this<br />

theory is used for selecting the optimal conditions for power input into a tokamak. The dependences<br />

of plasma density <strong>and</strong> temperature on the input power for auxiliary heating are found. Current ramp-up<br />

with lower hybrid waves <strong>and</strong> neutral beam injection is considered. It is shown that the current ramp-up<br />

rate, as a function of input power <strong>and</strong> plasma density, has a maximum. This allows either the current<br />

rise time or the energy consumption to be minimized at this stage. However, even in this optimized case<br />

the stage of current ramp-up in a tokamak of the reactor type turns out to be rather long.<br />

1. INTRODUCTION<br />

Gas ionization <strong>and</strong> current ramp-up are necessary elements in the discharge<br />

scenario. However, while there exists a great body of experience with the traditional<br />

inductive technique for discharge production, there are few experiments on the noninductive<br />

technique [1-5]. In inductive discharges the stages of gas ionization <strong>and</strong><br />

current ramp-up coincide in time <strong>and</strong>, as a rule, by the end of gas ionization there<br />

are closed magnetic surfaces in the tokamak chamber. The situation is different in<br />

the non-inductive tokamak. Gas ionization (hot plasma production) <strong>and</strong> current rampup<br />

can be performed by different methods <strong>and</strong> not necessarily at the same time. In<br />

this case, at the ionization stage closed magnetic surfaces can be absent from the<br />

plasma <strong>and</strong> the mechanisms of particle <strong>and</strong> energy confinement can be different, in<br />

principle, from the well studied case of inductive discharges.<br />

In this paper the stages of gas ionization <strong>and</strong> current ramp-up in the noninductive<br />

tokamak are considered. Our approach differs from that of all previous<br />

papers mainly in the use of the recently developed theory of plasma equilibrium in<br />

a toroidal magnetic system without rotational transform [6, 7]. As- shown in<br />

Refs [6, 7], toroidal drift, which has been considered as the main loss channel, being<br />

non-ambipolar, results in the emergence of a vertical electric field <strong>and</strong> in a toroidal<br />

739

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