High-Order Triangle-based Discontinuous Galerkin Methods for Hyperbolic
Equations on a Rotating Sphere
[postscript]
[PDF]
Animations of Shock Wave Dynamics on a Sphere
[Animated Gif]
Accepted in the Journal of Computational Physics
Vol 214, pp 447-465 (2006)
Francis X. Giraldo
Naval Research Laboratory
Monterey, CA 93943
ABSTRACT
High-order triangle-based discontinuous Galerkin (DG) methods for
hyperbolic equations on a rotating sphere are presented. The DG method can be characterized as the fusion of
finite elements with finite volumes. This DG formulation uses high-order Lagrange
polynomials on the triangle using nodal sets up to 15th order.
The finite element-type area
integrals are evaluated using order $2N$ Gauss cubature rules.
This leads to a full mass
matrix which, unlike for continuous Galerkin (CG) methods such as the
spectral element (SE) method presented in \cite{giraldo_2005b}, is small, local
and efficient to invert. Two types of finite volume-type
flux integrals are studied: a set based on Gauss-Lobatto quadrature points
(order $2N-1$) and a set based on Gauss quadrature points (order $2N$).
Furthermore, we explore conservation and advection forms as well as strong and weak
forms. Seven test cases are used to compare the different methods including
some with scale contractions and shock waves.
All three strong forms performed extremely well with the strong conservation form
with $2N$ integration being the most accurate of the four DG methods studied.
The strong advection form with $2N$ integration performed extremely well even
for flows with shock waves.
The strong conservation form with $2N-1$ integration yielded results almost as good as
those with $2N$ while being less expensive. All the DG methods
performed better than the SE method for almost all the test cases,
especially for those with strong discontinuities. Finally, the DG methods
required less computing time than the SE method due to the local nature of the
mass matrix.
Last Modified: August 2004