. "P(1M06031), P(IAA200760801), Z(AV0Z20760514)" . "RIV/61388998:_____/10:00353338" . . . . . "Stability of swirling annular flow"@en . "Mar\u0161\u00EDk, Franti\u0161ek" . . "Stability of swirling annular flow" . . "3" . . . "13"^^ . "Stability of swirling annular flow" . "swirling jet; hydrodynamic stability; impinging jet"@en . "Novotn\u00FD, Pavel" . . "[16A118F9D648]" . "Werner, E." . . "US - Spojen\u00E9 st\u00E1ty americk\u00E9" . . "289588" . . . "1065-3090" . . . . "Journal of flow visualization and image processing" . "17" . . . "Stability of swirling annular flow"@en . "RIV/61388998:_____/10:00353338!RIV11-MSM-61388998" . "3"^^ . "The influence of rotation on the stability of coaxial flow between steady cylinders is still an open question. The pattern of swirling annular jet depends strongly on the quality of the issuing flow. Our new approach to the fluid flow stability problem is based on the attenuation of the kinetic energy of disturbances. This concept follows from the thermodynamic stability conditions. To show the ability of this new concept we concentrate on an isothermal swirl flow in coaxial tube with constant density and viscosity."@en . "The influence of rotation on the stability of coaxial flow between steady cylinders is still an open question. The pattern of swirling annular jet depends strongly on the quality of the issuing flow. Our new approach to the fluid flow stability problem is based on the attenuation of the kinetic energy of disturbances. This concept follows from the thermodynamic stability conditions. To show the ability of this new concept we concentrate on an isothermal swirl flow in coaxial tube with constant density and viscosity." . . "Tr\u00E1vn\u00ED\u010Dek, Zden\u011Bk" . "4"^^ .