Page 120 - Fundamentals of Magnetic Thermonuclear Reactor Design
P. 120

104     Fundamentals of Magnetic Thermonuclear Reactor Design


            result for the tokamak as a whole) is found using the superposition principle.
            This algorithm enables a fourfold decrease in the computer memory allocated
            when solving problems with integral–differential problem formulation that
            implies dense matrices.
               The  TYPHOON  and  TORNADO  codes  contain  special  post-processing
            modules to obtain outputs for the periodicity element Ω .
                                                         
               A general solution of the form
                               j tot  =  j +  j ;
                                        2
                                    1
                               B tot  = B + B +  B ;
                                         2
                                             ext
                                     1
                                           j ×
                               f tot  =  f +  f + 1  B +  j ×  B , 1
                                                    2
                                                2
                                    1
                                        2
            where j  and j , j  are the eddy current total and partial densities, B  is
                   tot
                            2
                         1
                                                                        tot
            the total field, B  and B  are partial fields due to eddy currents, B  is the
                                 2
                                                                    ext
                          1
            external field, f  is the Lorentz force total density, and f  = j  × (B  + B ),
                                                                        ext
                         tot
                                                               1
                                                                    1
                                                           1
            f  × (B  + B ) are components of the Lorentz force total density. Subscripts
             2
                      ext
                  2
 jtot=j +j ;Btot=B +B +Bext;ftot=f 1  1 and 2 denote partial components determined when solving the two prob-
 1
 2
 1
 2
 +f +j ×B +j ×B ,  lems mentioned.
 2
 2
 1
 2
 1
               In some cases, one can apply the superposition principle to widened an-
            gular sectors up to 180 degrees to obtain a general solution. If the sector is
            regular, the problem dimensionality is reduced that allows the use of a refined
            FE meshes.
               The TYPHOON code allows volume forces to be transformed to a set of
            equivalent nodal loads. Then, the TYPHOON output files can be used directly
            as inputs for a subsequent stress analysis.
            4.4.4  3D Computational Models
            The conducting shell concept is unsuitable for a mathematical description of
            massive conductive structures, such as the divertor and blanket modules. In this
            case, a 3D solid-body simulation is required. As with other numerical models, a
            3D model has limitations associated with the mesh approximation for the initial
            stages of modelled EM transients. That is why additional models need to be
            developed. For example, a perfect conductor model is applicable to evaluate a
            field outside a conducting structure in the analysis of the initial stage of an EM
            transient when the skin effect is pronounced. Within certain approaches, local
            models are capable of providing an adequate assessment of EM response of the
            structures.
               The code TORNADO enables the analysis of EM transients in massive
            solids. The code uses four types of FEs: eight-node hexahedra, six-node
            triangular prisms, five-node pyramids, and four-node tetrahedra. Equations
            are solved in terms of the three-component electric vector potential P and
   115   116   117   118   119   120   121   122   123   124   125