International audienceFree-surface flows past submerged obstacles in a channel are considered. The fluid is assumed to be inviscid and incompressible and the flow to be irrotational. The first-order approximation of long nonlinear surface waves over one or two bumps results in a forced Korteweg-de Vries (fKdV) equation. Solutions of the stationary fKdV equation are constructed and their stability is studied, either analytically or numerically. These various solutions include solitary waves over a single bump, solitary waves with two humps over a double bump, table-top solutions over a double bump and fronts
The exact equations for surface waves over an uneven bottom can be formulated as a Hamiltonian syste...
The linearized Euler equations and the forced Korteweg-de Vries equation are investigated analytical...
The forced Korteweg-de Vries (KdV) equation is the KdV equation with a forcing term and arises as a ...
International audienceFree-surface flows past submerged obstacles in a channel are considered. The f...
The time independent surface waves on a two dimensional incompressible and inviscid fluid flow passi...
The time independent surface waves on a two dimensional incompressible and inviscid fluid flow passi...
The forced Korteweg-de Vries equation is considered to investigate the impact of bottom configuratio...
Two-dimensional free-surface flow past disturbances in an open channel is a classical problem in hyd...
Abstract. Surface waves at the free surface of an incompressible fluid passing over an obstruction a...
Flow over bottom topography at critical Froude number is examined with a focus on steady, forced sol...
The free-surface flow generated by multiple bumps at the bottom topography in a rectangular channel ...
Two-dimensional solitary waves generated by disturbances moving near the critical speed in shallow w...
Water waves phenomenon with a forcing disturbance causing unsteady waves is considered as a complica...
Very steep solitary waves on the surface of a flow in a channel have been widely studied, in part du...
The flow of water over an obstacle is a fundamental problem in fluid mechanics. Transcritical flow m...
The exact equations for surface waves over an uneven bottom can be formulated as a Hamiltonian syste...
The linearized Euler equations and the forced Korteweg-de Vries equation are investigated analytical...
The forced Korteweg-de Vries (KdV) equation is the KdV equation with a forcing term and arises as a ...
International audienceFree-surface flows past submerged obstacles in a channel are considered. The f...
The time independent surface waves on a two dimensional incompressible and inviscid fluid flow passi...
The time independent surface waves on a two dimensional incompressible and inviscid fluid flow passi...
The forced Korteweg-de Vries equation is considered to investigate the impact of bottom configuratio...
Two-dimensional free-surface flow past disturbances in an open channel is a classical problem in hyd...
Abstract. Surface waves at the free surface of an incompressible fluid passing over an obstruction a...
Flow over bottom topography at critical Froude number is examined with a focus on steady, forced sol...
The free-surface flow generated by multiple bumps at the bottom topography in a rectangular channel ...
Two-dimensional solitary waves generated by disturbances moving near the critical speed in shallow w...
Water waves phenomenon with a forcing disturbance causing unsteady waves is considered as a complica...
Very steep solitary waves on the surface of a flow in a channel have been widely studied, in part du...
The flow of water over an obstacle is a fundamental problem in fluid mechanics. Transcritical flow m...
The exact equations for surface waves over an uneven bottom can be formulated as a Hamiltonian syste...
The linearized Euler equations and the forced Korteweg-de Vries equation are investigated analytical...
The forced Korteweg-de Vries (KdV) equation is the KdV equation with a forcing term and arises as a ...