A very high-order finite volume method for the time-dependent convection-diffusion problem with Butcher Tableau extension

The time discretization of a very high-order nite volume method may give rise to new numerical diculties resulting into accuracy degradations. Indeed, for the simple onedimensional unstationary convection-diusi on equation for instance, a conicting situation between the source term time discretization and the boundary conditions may arise when using the standard Runge-Kutta method. We propose an alternative procedure by extending the Butcher Tableau to overcome this specic diculty and achieve fourth-, sixth- or eighth-order of accuracy schemes in space and time. To this end, a new nite volume method is designed based on specic polynomial reconstructions for the space discretization, while we use the Extended Butcher Tableau to perform the time discretization. A large set of numerical tests has been carried out to validate the proposed method.

[1]  Michael Dumbser,et al.  ADER-WENO finite volume schemes with space-time adaptive mesh refinement , 2012, J. Comput. Phys..

[2]  Praveen Chandrashekar,et al.  Vertex-centroid finite volume scheme on tetrahedral grids for conservation laws , 2011, Comput. Math. Appl..

[3]  Julio Hernández,et al.  High‐order finite volume schemes for the advection–diffusion equation , 2002 .

[4]  João M. Nóbrega,et al.  A sixth-order finite volume method for multidomain convection–diffusion problem with discontinuous coefficients , 2013 .

[5]  Stéphane Clain,et al.  Multi-dimensional Optimal Order Detection (MOOD) — a Very High-Order Finite Volume Scheme for Conservation Laws on Unstructured Meshes , 2011 .

[6]  Stéphane Clain,et al.  A high-order finite volume method for systems of conservation laws - Multi-dimensional Optimal Order Detection (MOOD) , 2011, J. Comput. Phys..

[7]  M. F.,et al.  Bibliography , 1985, Experimental Gerontology.

[8]  R. Eymard,et al.  Finite Volume Methods , 2019, Computational Methods for Fluid Dynamics.

[9]  Thierry Gallouët,et al.  The nite volume method , 2000 .

[10]  E. Bertolazzi,et al.  A unified treatment of boundary conditions in least-square based finite-volume methods , 2005 .

[11]  Clinton P. T. Groth,et al.  High-Order Solution-Adaptive Central Essentially Non-Oscillatory (CENO) Method for Viscous Flows , 2011 .

[12]  Clinton P. T. Groth,et al.  High-order solution-adaptive central essentially non-oscillatory (CENO) method for viscous flows , 2011, J. Comput. Phys..

[13]  Chi-Wang Shu,et al.  Strong Stability-Preserving High-Order Time Discretization Methods , 2001, SIAM Rev..

[14]  J. Lambert Numerical Methods for Ordinary Differential Equations , 1991 .

[15]  Eleuterio F. Toro,et al.  ADER finite volume schemes for nonlinear reaction--diffusion equations , 2009 .

[16]  C. Ollivier-Gooch,et al.  A high-order-accurate unstructured mesh finite-volume scheme for the advection-diffusion equation , 2002 .

[17]  Michael Dumbser,et al.  ADER Schemes for Nonlinear Systems of Stiff Advection–Diffusion–Reaction Equations , 2011, J. Sci. Comput..