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   <dc:title>EQUILI module in ALYA: a free-boundary GradShafranov equation solver using CutFEM</dc:title>
   <dc:title>Development of new EQUILI module for ALYA: implementation of a free-boundary solver for the Grad-Shafranov equation</dc:title>
   <dc:creator>Manyer i Fuertes, Pau</dc:creator>
   <dc:subject>Àrees temàtiques de la UPC::Matemàtiques i estadística::Anàlisi numèrica::Mètodes en elements finits</dc:subject>
   <dc:subject>Magnetohydrodynamics</dc:subject>
   <dc:subject>Finite element method</dc:subject>
   <dc:subject>High performance computing</dc:subject>
   <dc:subject>Plasma Equilirium</dc:subject>
   <dc:subject>Grad-Shafranov equations</dc:subject>
   <dc:subject>Alya Framework</dc:subject>
   <dc:subject>CutFem</dc:subject>
   <dc:subject>Magnetohidrodinàmica</dc:subject>
   <dc:subject>Elements finits, Mètode dels</dc:subject>
   <dc:subject>Càlcul intensiu (Informàtica)</dc:subject>
   <dcterms:abstract>The study of Magnetohydrodynamics (MHD) for plasma systems circulating in tokamaks is crucial for improving and developing more efficient and&#xd;
functional nuclear fusion reactors, advancing in the research of a new clean&#xd;
and sustainable source of energy. Nonetheless, MHD simulations must be&#xd;
provided with an initial configuration of the plasma, frequently based on the&#xd;
equilibrium state.&#xd;
The Grad-Shafranov equation models the equilibrium balancing the plasma&#xd;
pressure and the magnetic confinement in a nuclear reactor for an axisymmetrical plasma system, yielding as a result the poloidal magnetic flux ψ field&#xd;
used notably to visualise the shape of the magnetically confined plasma crosssection. Following guidelines from [1] and [2], EQUILI has been developed as&#xd;
a new independent and functional module inside the high performance computing (HPC) multiphysics Finite Elements (FE) code ALYA [3]. EQUILI&#xd;
solves for a given tokamak geometry the Grad-Shafranov equation using an&#xd;
iterative CutFEM solver.&#xd;
CutFEM is part of a branch of FE methods characterised by an unfitted&#xd;
computational mesh, where geometries and domains are embedded and interfaces are parametrized using level-set functions. This particular method is&#xd;
adapted for problems where interfaces are affected by large deformations and&#xd;
resizing, thus making it well-suited to address magnetically confined plasma&#xd;
equilibrium problems.&#xd;
While the tokamak’s confining magnets’ currents and positions can be individually adjusted to accommodate a variety of plasma pressure and current&#xd;
profiles in terms of plasma positioning and shaping, the current carried by&#xd;
the plasma depends directly on its cross-section shape, which at the same&#xd;
time is affected by the plasma current self-induced magnetic field. Due to&#xd;
this coupling, the problem needs to be solved using an iterative solver and&#xd;
having the plasma shape not fixed and free (free-boundary problem) to evolve&#xd;
towards the equilibrium configuration, while being constraint by its own circulating current. Therefore, the flexible and deformable nature of the plasma&#xd;
cross-section demands in fact the implementation of a FE method that can&#xd;
deal with this plasticity and must be able to easily track such changes in the&#xd;
plasma/vacuum interface geometry.&#xd;
The module was validated against several ITER equilibrium formulations&#xd;
and a rigorous sensibility test was performed, considering variations in the&#xd;
poloidal field coils’ currents conforming the axisymmetrical nuclear fusion&#xd;
reactor.</dcterms:abstract>
   <dcterms:issued>2024-10-17</dcterms:issued>
   <dc:type>Master thesis</dc:type>
   <dc:rights>http://creativecommons.org/licenses/by-nc-nd/4.0/</dc:rights>
   <dc:rights>Open Access</dc:rights>
   <dc:rights>Attribution-NonCommercial-NoDerivs 4.0 International</dc:rights>
   <dc:publisher>Universitat Politècnica de Catalunya</dc:publisher>
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