Abstract
A finite element method based on bicubic Bézier surfaces is
applied to the simulation of MHD instabilities relevant to magnetically
confined fusion. The major advantage of the new technique is that it
allows a natural way to implement mesh refinement strategy, which is not
supported by a pure Hermite formulation. Compared to a Lagrangian
formulation the number of degrees of freedom is significantly reduced.
The use of an isoparametric representation of the space coordinates
allows an accurate alignment of the finite elements to the magnetic
field line geometry in a tokamak plasma. The Bézier finite
elements have been implemented in a MHD code using the non-linear
reduced MHD model in toroidal geometry. As an illustration, results for
Soloviev equilibrium and time-dependent current-hole computations are
presented and discussed.
Original language | English |
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Pages (from-to) | 7423-7445 |
Journal | Journal of Computational Physics |
Volume | 227 |
Issue number | 16 |
DOIs | |
Publication status | Published - 1 Aug 2008 |
Externally published | Yes |