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1. magnetic confinement - ENEA - Fusione

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2. IGNITOR PROGRAM 59<br />

2.1 Introduction<br />

Pre-eminent among the significant events affecting the IGNITOR Project in 2001<br />

were the conclusions of the scientific debate initiated by the US fusion community<br />

when the U.S. withdrew from the ITER Project. These conclusions were summarised<br />

in the final report presented by the Fusion Energy Science Advisory Committee<br />

(FESAC) of the Department of Energy (DOE) [2.1]. The objective of the report was to<br />

provide the basis for proposing a programme for the next burning plasma<br />

experiment in the United States. The FESAC report clearly states that the only<br />

<strong>magnetic</strong> configuration sufficiently developed at this time to serve as a burning<br />

plasma experiment is the tokamak, and that all three burning plasma experimental<br />

designs today under development worldwide (IGNITOR, ITER-FEAT and FIRE)<br />

would deliver a large and significant advance in the understanding of burning plasma. This<br />

is an outstanding acknowledgement, at high international level, of the relevance of<br />

IGNITOR.<br />

[2.1] FESAC Panel Report<br />

on Burning Plasma Physics,<br />

Sept. 2001<br />

[2.2] G. Cenacchi, et al.,<br />

Bull. Am. Phys. Soc. 46,<br />

272 (2001)<br />

[2.3] A. Airoldi,et al., Bull.<br />

Am. Phys. Soc. 46, 271<br />

(2001)<br />

[2.4] G. Cenacchi, A.<br />

Airoldi: Equilibrium configurations<br />

for the<br />

Ignitor experiment, IFP<br />

report FP 01/1 (February<br />

2001)<br />

At <strong>ENEA</strong>, the design of the IGNITOR machine is sufficiently detailed to start the<br />

procurement of systems and components, once the Italian Government assures the funds<br />

for its construction and <strong>ENEA</strong> starts the licensing procedure. Meanwhile, the design work<br />

on this very compact, heavily loaded machine is being constantly updated to incorporate<br />

the latest progress in theoretical knowledge and experimental results in operating<br />

tokamaks. Technical specifications were issued to define the activity to be carried out with<br />

the support of industry and to update and revise the design of the main systems and<br />

components, and the relative contract is presently under negotiation with Ansaldo. In<br />

2001, the design activities concerned studies on the machine flexibility and advanced<br />

scenarios, the effect of new disruption data, the development of simplified engineering<br />

models for stress analysis of the nuclear core, plasma-wall interaction and impurity<br />

production studies and the design of the auxiliary ion cyclotron resonance heating (ICRH)<br />

system.<br />

2.2.1 Advanced scenarios<br />

2.2 Physics<br />

The poloidal field system is formed of 13+13 coils, symmetrically located relative to<br />

the machine equatorial plane and independently powered. The system is very<br />

flexible and allows X-point configurations as well as the limiter configurations of the<br />

reference scenario. Preliminary analyses, carried out with the equilibrium-transport<br />

code JETTO, concerned the possibility of obtaining high <strong>confinement</strong> conditions (the<br />

so-called “H-mode”) in the presence of double-null configurations around 10 MA<br />

and with auxiliary heating. The threshold power required for the L- to H-mode<br />

transition, evaluated according to the ITER scaling, is within the limits of the<br />

auxiliary heating system already included in the machine design [2.2]. The flat-top<br />

phase of the nominal IGNITOR scenario was analysed for situations in which a high<br />

impurity content delays ignition and leads to the development of sawtooth-type<br />

MHD instabilities [2.3].<br />

The MHD equilibrium configurations supporting the 11-MA 13-T IGNITOR scenario<br />

were carefully revised. The poloidal field coil currents required throughout the<br />

plasma evolution, from start-up to ignition, were determined both for the reference<br />

conditions and for the advanced scenario with the double null 10-MA configuration.<br />

Equilibrium configurations were obtained for both cases [2.4].<br />

2.3 Engineering of the Machine<br />

2.3.1 EM analysis of vacuum vessel during plasma disruptions<br />

The global forces induced on the IGNITOR vacuum vessel during plasma<br />

disruptions were estimated more precisely on the basis of the JET and Alcator C-Mod

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