. "Honz\u00E1tko, Radek" . . "Matematick\u00FD \u00FAstav AV \u010CR" . "composite scheme; dynamical effects; finite volume method"@en . "The work deals with a numerical solution of a 2D inviscid incompressible flow over a profile in a channel. The finite volume method in a form of cell-centered scheme is used. The composite scheme applied to a numerical solution consists of more dissipative part (Lax-Friedrichs scheme) and less dissipative part (Lax-Wendroff). Governing system of equations is the system of Euler equations. Two possibilities are considered. Firstly the flow is influenced by a prescribed oscillating behaviour of the profile. Secondly the oscillation of the profile is influenced by a flow field in the channel. In both cases the profile is fixed in the centre of gravity." . . "Numerical Solution of Unsteady Flow over a Profile in a Channel"@en . . "Praha" . . "Programy a algoritmy numerick\u00E9 matematiky 11" . "2"^^ . "RIV/68407700:21220/02:02087658" . . . "3"^^ . . . . . . "Hor\u00E1\u010Dek, Jarom\u00EDr" . . "80-85823-49-7" . "2003-06-09+02:00"^^ . "Numerical Solution of Unsteady Flow over a Profile in a Channel" . . "Numerical Solution of Unsteady Flow over a Profile in a Channel" . "8"^^ . "[FE41F929DB20]" . "Doln\u00ED Maxov" . . "65 ; 72" . "Numerical Solution of Unsteady Flow over a Profile in a Channel"@en . "P(GA101/02/0391), P(GA201/02/0684), P(GV101/98/K001), Z(MSM 210000010)" . "RIV/68407700:21220/02:02087658!RIV/2004/MSM/212204/N" . "Kozel, Karel" . . "656197" . "21220" . . . . . . "The work deals with a numerical solution of a 2D inviscid incompressible flow over a profile in a channel. The finite volume method in a form of cell-centered scheme is used. The composite scheme applied to a numerical solution consists of more dissipative part (Lax-Friedrichs scheme) and less dissipative part (Lax-Wendroff). Governing system of equations is the system of Euler equations. Two possibilities are considered. Firstly the flow is influenced by a prescribed oscillating behaviour of the profile. Secondly the oscillation of the profile is influenced by a flow field in the channel. In both cases the profile is fixed in the centre of gravity."@en .