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Mechanics of Magnetic Fusion Reactors  Chapter | 12    355


             field coil system, and controlled power supply to the CS and poloidal field coils
             at different discharge stages, including potential plasma disruptions. In addi-
             tion, there is a coil cooling stage in the superconducting magnet system (MS).
             These loads are taken up by load-bearing and support structures.
                Gen-1 and Gen-2 tokamaks (T-3, T-7, T-10, TFTR, etc.) employed regular
             ring-shaped TFCs, selected for fabrication simplicity. However, the non-uni-
             form in-plane ponderomotive forces cause extension and in-plane bending of
             the coil. It is therefore reasonable to utilise a D-shaped TFC, satisfying

                                        q ρ = const,                                                                qρ=const,
             where q is the linear load on the coil and ρ is the coil curvature radius. D-shaped
             (or close to being D-shaped) TFCs are used in JET, DOUBLET-III, KSTAR
             and other machines. D-shaped TFCs have been chosen for ITER.
                The strength criteria are important but not exclusive for selecting the TFC
             geometry. The most critical considerations are generally related to plasma phys-
             ics factors and operating needs.
                The poloidal field and CS coils are ring-shaped: a design feature allowing
             accommodation of the axis-symmetrical ponderomotive forces. Radial forces
             in toroidal systems are accommodated by either a central support cylinder or
             by wedging (‘barrel vault’). In the latter case, a continuous support cylinder is
             formed by the TFC’s straight parts. It transforms radial forces directed towards
             the tokamak centre into circumferential forces. Actually, a combination of the
             two solutions can be used.
                In large tokamaks, intercoil structures joining outer TFC blocks together
             take up the out-of-plane forces. The structures are segmented and connected at
             edges with keys and bolts to transmit shear forces. Horizontal keys take up the
             overturn moment, M , and vertical keys resist the torsional moment, M , and
                              R
                                                                       Z
             toroidal force, F  (Fig. 12.2). Out-of-plane forces can be additionally accom-
                          T
             modated by shell structures and external load-bearing frames.


















             FIGURE 12.2  Accommodation of forces acting in the TFC plane. (A) The radial moment and
             (B) the vertical moment and the toroidal force.
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