Related Experiment Video
Updated: Feb 17, 2026

08:54
Measurements of Waves in a Wind-wave Tank Under Steady and Time-varying Wind Forcing
Published on: February 13, 2018
9.1K
New exact relations for steady irrotational two-dimensional gravity and capillary surface waves
1Université Côte d'Azur, CNRS-LJAD UMR 7351, Parc Valrose, 06108 Nice, France didierc@unice.fr.
Summary
Researchers derived new exact equations for surface capillary-gravity waves using holomorphic properties. This work provides a new physical plane counterpart to the Babenko equation for nonlinear water waves.
Area of Science:
- Fluid dynamics
- Nonlinear wave theory
- Mathematical physics
Background:
- Surface capillary-gravity waves are fundamental in fluid dynamics.
- Understanding nonlinear water waves is crucial for various applications.
- Previous studies often involve complex mathematical formulations.
Purpose of the Study:
- To derive new exact relations and equations for steady 2D surface capillary-gravity waves.
- To obtain a physical plane counterpart of the Babenko equation.
- To simplify the analysis of nonlinear water waves.
Main Methods:
- Exploiting holomorphic properties in the physical plane.
- Transforming boundary conditions at the free surface.
- Deriving equations solely for the free surface dynamics.
Main Results:
- New exact relations for free surface waves were derived.
- A physical plane equivalent of the Babenko equation was obtained.
- The study focuses on constant depth conditions.
Conclusions:
- The derived equations offer a simplified approach to studying nonlinear water waves.
- This work contributes to the understanding of capillary-gravity wave dynamics.
- The findings are relevant to the theme issue on Nonlinear water waves.
More Related Videos
Related Concept Videos
Navier–Stokes Equations
2.3K
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
2.3K
Steady, Laminar Flow Between Parallel Plates
900
Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
900
Irrotational Flow
1.0K
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
1.0K
Euler's Equations of Motion
958
In fluid mechanics, shear stresses arise from viscosity, which represents a fluid's internal resistance to deformation. For low-viscosity fluids, like water, these stresses are minimal, simplifying flow analysis by allowing the fluid to be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent, leaving only normal stresses, which act perpendicularly to fluid elements. Notably, pressure — defined as the negative of the normal stress — remains uniform across...
958
Steady, Laminar Flow in Circular Tubes
1.2K
Hagen-Poiseuille flow describes a viscous fluid's steady, incompressible flow through a cylindrical tube with a constant radius R. This flow profile is often applied to understand fluid transport in narrow channels, such as capillaries. It serves as a foundational example of laminar flow. In this model, cylindrical coordinates (r,θ,z) are used to describe the radial (r), angular (θ), and axial (z) dimensions within the tube. For Hagen-Poiseuille flow, the velocity profile is purely axial,...
1.2K
Newtonian Fluid: Problem Solving
1.0K
Newtonian fluids exhibit a constant viscosity, meaning their shear stress and shear strain rate are directly proportional. This property ensures a predictable and stable response to applied forces, maintaining a linear relationship between force and flow. Examples include water, air, and light oils, consistently demonstrating this proportional behavior regardless of external conditions.
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
1.0K

