SummaryFinite elements of class are suitable for the computation of magnetohydrodynamics instabilities in tokamak plasmas. In addition, isoparametric approximations allow for a precise alignment of the mesh with the magnetic field line. Mesh alignment is crucial to achieve axisymmetric equilibria accurately. It is also helpful to deal with the anisotropy nature of magnetized plasma flows. In this numerical framework, several practical simulations are now available. They help to understand better the operation of existing devices and predict the optimal strategies for using the international ITER tokamak under construction. However, a meshâaligned isoparametric representation suffers from the presence of critical points of the magnetic field (magnetic axis, Xâpoint). We here explore a strategy that combines aligned mesh out of the critical points with nonâaligned unstructured mesh in a region containing these points. By this strategy, we can avoid highly stretched elements and the numerical difficulties that come with them. The meshâaligned interpolation uses biâcubic HemiteâBĂ©zier polynomials on a structured mesh of curved quadrangular elements. On the other hand, we assume reduced cubic HsiehâCloughâTocher finite elements on an unstructured triangular mesh. Both meshes overlap, and the resulting formulation is a coupled discrete problem solved iteratively by a suitable oneâlevel Schwarz algorithm. In this paper, we will focus on the Poisson problem on a twoâdimensional bounded regular domain. This elliptic equation is a simplified version of the axisymmetric tokamak equilibrium one at the asymptotic limit of infinite major radius (large aspect ratio).