ENTROPY STABLE APPROXIMATIONS OF NAVIER–STOKES EQUATIONS WITH NO ARTIFICIAL NUMERICAL VISCOSITY

2006 ◽  
Vol 03 (03) ◽  
pp. 529-559 ◽  
Author(s):  
EITAN TADMOR ◽  
WEIGANG ZHONG

We construct a new family of entropy stable difference schemes which retain the precise entropy decay of the Navier–Stokes equations, [Formula: see text] To this end we employ the entropy conservative differences of [24] to discretize Euler convective fluxes, and centered differences to discretize the dissipative fluxes of viscosity and heat conduction. The resulting difference schemes contain no artificial numerical viscosity in the sense that their entropy dissipation is dictated solely by viscous and heat fluxes. Numerical experiments provide a remarkable evidence for the different roles of viscosity and heat conduction in forming sharp monotone profiles in the immediate neighborhoods of shocks and contacts.

2014 ◽  
Vol 36 (5) ◽  
pp. B835-B867 ◽  
Author(s):  
Mark H. Carpenter ◽  
Travis C. Fisher ◽  
Eric J. Nielsen ◽  
Steven H. Frankel

2016 ◽  
Vol 20 (suppl. 3) ◽  
pp. 853-858
Author(s):  
Zhi-Jun Meng ◽  
Yao-Ming Zhou ◽  
Dong-Mu Mei

This paper addresses the systems of the incompressible Navier-Stokes equations on Cantor sets without the external force involving the fractal heat-conduction problem vial local fractional derivative. The spherical Cantor type co-ordinate method is used to transfer the incompressible Navier-Stokes equation from the Cantorian co-ordinate system into the spherical Cantor type co-ordinate system.


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