Abstract
Many problems in biology and engineering are governed by anisotropic reactiondiffusion equations with
a very rapidly varying reaction term. These characteristics of the system imply the use of very fine meshes
and small time steps in order to accurately capture the propagating wave avoiding the appearance of
spurious oscillations in the wave front. This work develops a fourth-order compact scheme for anisotropic
reactiondiffusion equations with stiff reactive terms. As mentioned, the scheme accounts for the anisotropy
of the media and incorporates an adaptive time step for handling the stiff reactive term. The high-order
scheme allows working with coarser meshes without compromising numerical accuracy rendering a more
efficient numerical algorithm by reducing the total computation time and memory requirements. The order
of convergence of the method has been demonstrated on an analytical solution with Neumann boundary
conditions. The scheme has also been implemented for the solution of anisotropic electrophysiology
problems. Anisotropic square samples of normal and ischemic cardiac tissue have been simulated by means
of the monodomain model with the reactive term defined by LuoRudy II dynamics. The simulations
proved the effectiveness of the method in handling anisotropic heterogeneous non-linear reactiondiffusion
problems. Bidimensional tests also indicate that the fourth-order scheme requires meshes about 45%
coarser than the standard second-order method in order to achieve the same accuracy of the results.