Article information

1997 , Volume 2, ¹ 6, p.53-60

Martyushov S.N.

Calculation of two-dimensional diffraction by Harten algorithm of the second order of accuracy

The Harten`s difference algorithm of the second order of accuracy has been realised by the finite volume method in a three-dimensional, two-dimensional plane and axially symmetrical statements with respect to space and time variables. On realising the algorithm the following modifications have been performed: pseudo-characteristic eigenvectors were introduced, the additional bounder of the artifical compression operator was determined, a simplified function of artifical viscosity is used. The Harten`s operator bounders (with additional compresion) and Royer`s (Superbee) are employed. The two-dimensional calculations grids are constructed on the basis of Thompson`s algorithm consisting in the solving of the vector Poisson equation. The geometrical adaptation of the grids is attained by the suitable selection of corresponding coefficients in the control functions i.e. the right-hand sides of the Poisson equation. Three two-dimensional were calculated: the outlet of an axially jet from a cylindrical nozzle; the shock wave diffraction on a convex angle, transition from the regular Mach and double Mach non-stationary reflection under interaction of the plane shock wave with a convex surface.

[full text] Classificator Msc2000:
*76J20 Supersonic flows
76L05 Shock waves and blast waves
76M20 Finite difference methods

Keywords: Mach reflection, supersonic flow, alpha-variant of Harten scheme, cylindrical nozzle, shock wave diffraction, regular reflection, Euler equations, inviscid perfect gas, vector Poisson equation, Thompson algorithm

Author(s):
Martyushov Sergei Nikolaevich
PhD. , Senior Scientist
Address: 125222, Russia, Moscow
Phone Office: (495) 692 40 78
E-mail: martyush@mail.ru


Bibliography link:
Martyushov S.N. Calculation of two-dimensional diffraction by Harten algorithm of the second order of accuracy // Computational technologies. 1997. V. 2. ¹ 6. P. 53-60
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