1. magnetic confinement - ENEA - Fusione
1. magnetic confinement - ENEA - Fusione
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