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Davey–Stewartson equation

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In fluid dynamics, the Davey–Stewartson equation (DSE) was introduced in a paper by Davey & Stewartson (1974) to describe the evolution of a three-dimensional wave-packet on water of finite depth.

It is a system of partial differential equations for a complex (wave-amplitude) field u and a real (mean-flow) field ϕ :

i u t + c 0 u x x + u y y = c 1 | u | 2 u + c 2 u ϕ x , ϕ x x + c 3 ϕ y y = ( | u | 2 ) x .

The DSE is an example of a soliton equation in 2+1 dimensions. The corresponding Lax representation for it is given in Boiti, Martina & Pempinelli (1995).

In 1+1 dimensions the DSE reduces to the nonlinear Schrödinger equation

i u t + u x x + 2 k | u | 2 u = 0.

Itself, the DSE is the particular reduction of the Zakharov–Schulman system. On the other hand, the equivalent counterpart of the DSE is the Ishimori equation.

The DSE is the result of a multiple-scale analysis of modulated nonlinear surface gravity waves, propagating over a horizontal sea bed.

References

Davey–Stewartson equation Wikipedia