In fluid dynamics, the Falkner–Skan boundary layer (named after V. M. Falkner and Sylvia W. Skan) describes the steady two-dimensional laminar boundary layer that forms on a wedge, i.e. flows in which the plate is not parallel to the flow. It is also representative of flow on a flat plate with an imposed pressure gradient along the plate length, a situation often encountered in wind tunnel flow. It is a generalization of the flat plate Blasius boundary layer in which the pressure gradient along the plate is zero.
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| - Falkner–Skan boundary layer (en)
- Équation de Falkner-Skan (fr)
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| - In fluid dynamics, the Falkner–Skan boundary layer (named after V. M. Falkner and Sylvia W. Skan) describes the steady two-dimensional laminar boundary layer that forms on a wedge, i.e. flows in which the plate is not parallel to the flow. It is also representative of flow on a flat plate with an imposed pressure gradient along the plate length, a situation often encountered in wind tunnel flow. It is a generalization of the flat plate Blasius boundary layer in which the pressure gradient along the plate is zero. (en)
- L'équation de Falkner-Skan est une équation différentielle solution de l'écoulement potentiel sur un dièdre. Elle généralise l'équation de Blasius pour la plaque plane et la solution de Hiemenz pour le point d'arrêt en écoulement bidimensionnel. Elle a été établie par V. M. Falkner et Sylvia Skan en 1930. (fr)
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| - In fluid dynamics, the Falkner–Skan boundary layer (named after V. M. Falkner and Sylvia W. Skan) describes the steady two-dimensional laminar boundary layer that forms on a wedge, i.e. flows in which the plate is not parallel to the flow. It is also representative of flow on a flat plate with an imposed pressure gradient along the plate length, a situation often encountered in wind tunnel flow. It is a generalization of the flat plate Blasius boundary layer in which the pressure gradient along the plate is zero. (en)
- L'équation de Falkner-Skan est une équation différentielle solution de l'écoulement potentiel sur un dièdre. Elle généralise l'équation de Blasius pour la plaque plane et la solution de Hiemenz pour le point d'arrêt en écoulement bidimensionnel. Elle a été établie par V. M. Falkner et Sylvia Skan en 1930. (fr)
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