2022Unpublished venueRequires access

The Korteweg–de Vries Equation

Ahmed Lesfari

Open publisher page 6 citations

Abstract

The Korteweg–de Vries (KdV) equation, which is a nonlinear partial differential equation of the third order, is a universal mathematical model for the description of weakly nonlinear long wave propagation in dispersive media. This chapter aims to study the KdV equation and the inverse scattering method (based on Schrodinger and Gelfand–Levitan equations) used to solve it. The KdV equation preserves mass, momentum, energy and many other quantities. The nonlinear KdV equation is transformed into the linear Gelfand–Levitan equation. The spectrum of the Schrodinger operator is invariant by the Hamiltonian flow defined by the KdV equation. The isospectral sets related to invariant manifolds defined by putting these invariants equal to generic constants are compact, connected and infinite-dimensional tori.

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What this paper is about

The Korteweg–de Vries (KdV) equation, which is a nonlinear partial differential equation of the third order, is a universal mathematical model for the description of weakly nonlinear long wave propagation in dispersive media. This chapter aims to study the KdV equation and the inverse scattering method (based on Schrodinger and Gelfand–Levitan equations) used to solve it. The KdV equation preserves mass, momentum, energy and many other quantities. The nonlinear KdV equation is transformed into the linear Gelfand–Levitan equation. The spectrum of the Schrodinger operator is invariant by the Hamiltonian flow defined by the KdV equation. The isospectral sets related to invariant manifolds defined by putting these invariants equal to generic constants are compact, connected and infinite-dimensional tori.

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Available abstract

The Korteweg–de Vries (KdV) equation, which is a nonlinear partial differential equation of the third order, is a universal mathematical model for the description of weakly nonlinear long wave propagation in dispersive media. This chapter aims to study the KdV equation and the inverse scattering method (based on Schrodinger and Gelfand–Levitan equations) used to solve it. The KdV equation preserves mass, momentum, energy and many other quantities. The nonlinear KdV equation is transformed into the linear Gelfand–Levitan equation. The spectrum of the Schrodinger operator is invariant by the Hamiltonian flow defined by the KdV equation. The isospectral sets related to invariant manifolds defined by putting these invariants equal to generic constants are compact, connected and infinite-dimensional tori.

Key concepts: Korteweg–de Vries equation, Isospectral, Dispersionless equation, Mathematics, Inverse scattering transform, Nonlinear Schrödinger equation, Mathematical physics, Kadomtsev–Petviashvili equation

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