. "Kozel, Karel" . "Dynamical and Aeroelastic Effects in a Numerical Solution of Flow through a Cascade and over a Profile" . "Praha" . "Proceedings of the International Conference Mathematical and Computer Modelling in Science and Engineering" . "3"^^ . "Praha" . "Dynamical and Aeroelastic Effects in a Numerical Solution of Flow through a Cascade and over a Profile"@en . "Nen\u00ED k dispozici"@cs . . "604673" . "Dynamical and Aeroelastic Effects in a Numerical Solution of Flow through a Cascade and over a Profile"@en . "\u010Cesk\u00E9 vysok\u00E9 u\u010Den\u00ED technick\u00E9 v Praze" . "Hor\u00E1\u010Dek, Jarom\u00EDr" . "21220" . . "P(GA101/02/0391), P(GA201/02/0684), Z(MSM 210000010)" . "Nen\u00ED k dispozici"@cs . . . . "Nen\u00ED k dispozici"@cs . "152 ; 156" . "Honz\u00E1tko, Radek" . . . . "RIV/68407700:21220/03:02085812!RIV07-GA0-21220___" . "5"^^ . "2003-01-27+01:00"^^ . . . "The work deals with a numerical solution of 2D inviscid incompressible flow through a cascade and over a profile in a channel. The finite volume method in a form of cell-centered scheme at triangular and qudrilateral mesh is used. The composite scheme applied to a numerical solution consists of more dissipative part (Lax-Friedrichs scheme) and less dissipative part (Lax-Wendroff scheme). 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." . "RIV/68407700:21220/03:02085812" . "[7B39F0CBA906]" . . . . . . . . "The work deals with a numerical solution of 2D inviscid incompressible flow through a cascade and over a profile in a channel. The finite volume method in a form of cell-centered scheme at triangular and qudrilateral mesh is used. The composite scheme applied to a numerical solution consists of more dissipative part (Lax-Friedrichs scheme) and less dissipative part (Lax-Wendroff scheme). 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 . "2"^^ . . . "Dynamical and Aeroelastic Effects in a Numerical Solution of Flow through a Cascade and over a Profile" . "composite scheme; dynamical effects; finite volume method"@en . "80-7015-912-X" .