Discontinuous Galerkin Method for 1D Shallow Water Flow with Water Surface Slope Limiter

A water surface slope limiting scheme is tested and compared with the water depth slope limiter for the solution of one dimensional shallow water equations with bottom slope source term. Numerical schemes based on the total variation diminishing Runge- Kutta discontinuous Galerkin finite element method with slope limiter schemes based on water surface slope and water depth are used to solve one-dimensional shallow water equations. For each slope limiter, three different Riemann solvers based on HLL, LF, and Roe flux functions are used. The proposed water surface based slope limiter scheme is easy to implement and shows better conservation property compared to the slope limiter based on water depth. Of the three flux functions, the Roe approximation provides the best results while the LF function proves to be least suitable when used with either slope limiter scheme.

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References:
[1] J. S. Wang, H. G. Ni and Y. S. He, "Finite-difference TVD scheme for
computation of dam-break problems," J. Hydr. Engng., vol. 126, no. 4,
pp. 253-262, 2000.
[2] G. F. Lin, J. S. Lai and W. D. Guo, "Finite-volume component-wise
TVD schemes for 2D shallow water equations," Adv. Water Resour.,
vol. 26, no. 8, pp. 861-873, 2003.
[3] T. J. R. Hughes, W. K. Liu and A. Brooks, "Finite element analysis of
incompressible viscous flows by the penalty function formulation," J.
Comput. Phys., vol. 30, no. 1, pp. 1-60, 1979.
[4] O. C. Zienkiewicz and P. Ortiz, "A split-characteristic based finite
element model for the shallow equations," Int. J. Numer. Methods
Fluids, vol. 20, no. 8-9, pp. 1061-1080, 1995.
[5] T. Arbogast and M. F. Wheeler, "A characteristics-mixed finite element
method for advection-dominated transport problems," SIAM J. Numer.
Anal., vol. 32, no. 2, pp. 404-424, 1995.
[6] W. H. Reed and T. Hill, "Triangular Mesh Method for the Neutron
Transport Equation," Los Alamos Report, LA-UR-73-479, 1973.
[7] B. Cockburn and C. W. Shu, "TVB Runge-Kutta local projection
discontinuous Galerkin finite element method for conservation laws II:
General framework," Math. Comp., vol. 52, pp. 411-435, 1989.
[8] B. Cockburn, S. Y. Lin and C. W. Shu, "TVB Runge-Kutta local
projection discontinuous Galerkin finite element method for
conservation laws III: One dimensional systems," J. Comput. Phys, vol.
84, no. 1, pp. 90-113, 1989.
[9] B. Cockburn, S. Hou and C. W. Shu, "The Runge-Kutta local projection
discontinuous Galerkin finite element method for conservation laws. IV:
The multidimensional case," Math. Comp., vol. 54, pp. 545-581, 1990.
[10] B. Cockburn and C. W. Shu, "The Runge-Kutta discontinuous Galerkin
finite element method for conservation laws V: Multidimensional
systems," J. Comput. Phys., vol. 141, no. 2, pp. 199-224, 1998.
[11] B. Q. Li, "Discontinuous Finite Elements in Fluid Dynamics and Heat
Transfer," Springer Verlag, 2006.
[12] D. Schwanenberg and J. Köngeter, "A discontinuous Galerkin method
for the shallow water equations with source terms," Lecture Notes in
Computational Science and Engineering, Springer, Berlin, vol. 11, pp.
419-424, 2000.
[13] D. Schwanenberg and M. Harms, "Discontinuous Galerkin finiteelement
method for transcritical two-dimensional shallow water flows,"
J. Hydr. Engng., vol. 130, no. 5, pp. 412-421, 2004.
[14] V. Aizinger and C. Dawson, "A discontinuous Galerkin method for twodimensional
flow and transport in shallow water," Adv. Water Resour.,
vol. 25, no. 1, pp. 67-84, 2002.
[15] C. Dawson and V. Aizinger, "A discontinuous Galerkin method for
three-dimensional shallow water equations," J. Sci. Comput., vol. 22, no.
1, pp. 245-267, 2005.
[16] E. J. Kubatko, J. J. Westerink and C. Dawson, "hp discontinuous
Galerkin methods for advection dominated problems in shallow water
flow," Comput. Methods Appl. Mech. Eng., vol. 196, no, 1-3, pp. 437-
451, 2006.
[17] A. Harten, P. D. Lax and B. van Leer, "On upstream differencing and
Godunov-type schemes for hyperbolic conservation laws," SIAM Rev.,
vol. 25, no. 1, pp. 35-61, 1983.
[18] P. Roe, "Approximate Riemann solvers, parameter vectors, and
difference schemes," J. Comput. Phys., vol. 43, no. 2, pp. 357-372, 1981.
[19] P. Tassi, O. Bokhove and C. Vionnet, "Space discontinuous Galerkin
method for shallow water flowsÔÇökinetic and HLLC flux, and potential
vorticity generation," Adv. Water Resour., vol. 30, no. 4, pp. 998-1015,
2007.
[20] S. Gottlieb and C. W. Shu, "Total variation diminishing Runge-Kutta
schemes," Math. Comp., vol. 67, 73-85, 1998.
[21] J. G. Zhou, D. M. Causon, C. G. Mingham and D. M. Ingram, "The
surface gradient method for the treatment of source terms in the shallowwater
equations," J. Comput. Phys., vol. 168, no. 1, pp. 1-25, 2001.
[22] X. Ying, A. A. Khan and S. S. Y. Wang, "Upwind conservative scheme
for the Saint Venant equations," J. Hydr. Engng., vol. 130, no. 4, pp.
977-987, 2004.
[23] M. Catella, E. Paris and L. Solari, "Conservative scheme for numerical
modeling of flow in natural geometry," J. Hydr. Engng., vol. 134, no. 6,
pp. 736-748, 2008.
[24] B. Cockburn, "Discontinuous Galerkin Methods for Convection
Dominated Problems," Lecture Notes in Computational Science and
Engineering, Springer, Berlin, vol. 9, pp. 69-224, 2001.