%0 Journal Article %1 wu1994equation %A Wu, Jiankang %D 1994 %J International Journal for Numerical Methods in Engineering %K 35l05-wave-equation 76m10-finite-element-methods-in-fluid-mechanics 76m25-other-numerical-methods-in-fluid-mechanics 76r05-forced-convection 76r99-diffusion-and-convection %N 16 %P 2717-2733 %R 10.1002/nme.1620371603 %T Wave equation model for solving advection-diffusion equation %U https://onlinelibrary.wiley.com/doi/10.1002/nme.1620371603 %V 37 %X This paper presents a Wave Equation Model (WEM) to solve advection dominant Advection–Diffusion (A–D) equation. It is known that the operator-splitting approach is one of the effective methods to solve A–D equation. In the advection step the numerical solution of the advection equation is often troubled by numerical dispersion or numerical diffusion. Instead of directly solving the first-order advection equation, the present wave equation model solves a second-order equivalent wave equation whose solution is identical to that of the first-order advection equation. Numerical examples of 1-D and 2-D with constant flow velocities and varying flow velocities are presented. The truncation error and stability condition of 1-D wave equation model is given. The Fourier analysis of WEM is carried out. The numerical solutions are in good agreement with the exact solutions. The wave equation model introduces very little numerical oscillation. The numerical diffusion introduced by WEM is cancelled by inverse numerical diffusion introduced by WEM as well. It is found that the numerical solutions of WEM are not sensitive to Courant number under stability constraint. The computational cost is economical for practical applications.

@article{wu1994equation, abstract = { This paper presents a Wave Equation Model (WEM) to solve advection dominant Advection–Diffusion (A–D) equation. It is known that the operator-splitting approach is one of the effective methods to solve A–D equation. In the advection step the numerical solution of the advection equation is often troubled by numerical dispersion or numerical diffusion. Instead of directly solving the first-order advection equation, the present wave equation model solves a second-order equivalent wave equation whose solution is identical to that of the first-order advection equation. Numerical examples of 1-D and 2-D with constant flow velocities and varying flow velocities are presented. The truncation error and stability condition of 1-D wave equation model is given. The Fourier analysis of WEM is carried out. The numerical solutions are in good agreement with the exact solutions. The wave equation model introduces very little numerical oscillation. The numerical diffusion introduced by WEM is cancelled by inverse numerical diffusion introduced by WEM as well. It is found that the numerical solutions of WEM are not sensitive to Courant number under stability constraint. The computational cost is economical for practical applications.}, added-at = {2021-08-02T01:56:37.000+0200}, author = {Wu, Jiankang}, biburl = {https://www.bibsonomy.org/bibtex/2a4f56bfecc68bc87fdfd549a7819ce9a/gdmcbain}, doi = {10.1002/nme.1620371603}, interhash = {978c2d0f56e753294c369acc695b5b2c}, intrahash = {a4f56bfecc68bc87fdfd549a7819ce9a}, journal = {International Journal for Numerical Methods in Engineering}, keywords = {35l05-wave-equation 76m10-finite-element-methods-in-fluid-mechanics 76m25-other-numerical-methods-in-fluid-mechanics 76r05-forced-convection 76r99-diffusion-and-convection}, number = 16, pages = {2717-2733}, timestamp = {2021-08-02T01:58:18.000+0200}, title = {Wave equation model for solving advection-diffusion equation}, url = {https://onlinelibrary.wiley.com/doi/10.1002/nme.1620371603}, volume = 37, year = 1994 }