A general-purpose finite-volume advection scheme for continuous and discontinuous fields on unstructured grids

  • Authors:
  • E. D. Dendy;N. T. Padial-Collins;W. B. VanderHeyden

  • Affiliations:
  • Los Alamos National Laboratory, Theoretical Division, Fluid Dynamics Group (T-3), and Los Alamos Computer Science Institute, Los Alamos, New Mexico;Los Alamos National Laboratory, Theoretical Division, Fluid Dynamics Group (T-3), and Los Alamos Computer Science Institute, Los Alamos, New Mexico;Los Alamos National Laboratory, Theoretical Division, Fluid Dynamics Group (T-3), and Los Alamos Computer Science Institute, Los Alamos, New Mexico

  • Venue:
  • Journal of Computational Physics
  • Year:
  • 2002

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Abstract

We present a new general-purpose advection scheme for unstructured meshes based on the use of a variation of the interface-tracking flux formulation recently put forward by O. Ubbink and R. I. Issa (J. Comput. Phys. 153, 26 (1999)), in combination with an extended version of the flux-limited advection scheme of J. Thuburn (J. Comput. Phys. 123, 74 (1996)), for continuous fields. Thus, along with a high-order mode for continuous fields, the new scheme presented here includes optional integrated interface-tracking modes for discontinuous fields. In all modes, the method is conservative, monotonic, and compatible. It is also highly shape preserving. The scheme works on unstructured meshes composed of any kind of connectivity element, including triangular and quadrilateral elements in two dimensions and tetrahedral and hexahedral elements in three dimensions. The scheme is finite-volume based and is applicable to control-volume finite-element and edge-based node-centered computations. An explicit-implicit extension to the continuous-field scheme is provided only to allow for computations in which the local Courant number exceeds unity. The transition from the explicit mode to the implicit mode is performed locally and in a continuous fashion, providing a smooth hybrid explicit-implicit calculation. Results for a variety of test problems utilizing the continuous and discontinuous advection schemes are presented.