M. Ferrari et al., IMPACT OF THE PASSIVE STABILIZATION SYSTEM ON THE DYNAMIC LOADS OF THE ITER FIRST WALL BLANKET DURING A PLASMA DISRUPTION EVENT/, Fusion engineering and design, 27, 1995, pp. 507-514
In next-generation tokamak devices (i.e. ITER), passive stabilization
of the plasma is required to mitigate the consequences of the plasma v
ertical displacements and to reduce the occurrence of plasma disruptio
ns. With this aim, two main design approaches have been considered. Th
e first one (adopted in the ITER CDA design) consists of copper stabil
ization loops (twin loops) attached to box-shaped blanket segments whi
ch are electrically and mechanically separated along the toroidal dire
ction. In the second design approach (under consideration for the ITER
EDA design), relying on a lower plasma elongation, no specific stabil
ization loops are required and the passive stabilization is achieved b
y toroidally continuous components, in particular by the plasma facing
wall of the blanket segments, electrically connected along the toroid
al direction, thus allowing a toroidal current to flow during the elec
tromagnetic transients. In both cases electrodynamic loads arise in th
e blanket structures during plasma disruptions and/or vertical displac
ement events, A comparison between the two design approaches has been
carried out from the eddy-current and related load distribution viewpo
int.