Search results for "Dispersive partial differential equation"

showing 2 items of 2 documents

Numerical study of a multiscale expansion of the Korteweg de Vries equation and Painlev\'e-II equation

2007

The Cauchy problem for the Korteweg de Vries (KdV) equation with small dispersion of order $\e^2$, $\e\ll 1$, is characterized by the appearance of a zone of rapid modulated oscillations. These oscillations are approximately described by the elliptic solution of KdV where the amplitude, wave-number and frequency are not constant but evolve according to the Whitham equations. Whereas the difference between the KdV and the asymptotic solution decreases as $\epsilon$ in the interior of the Whitham oscillatory zone, it is known to be only of order $\epsilon^{1/3}$ near the leading edge of this zone. To obtain a more accurate description near the leading edge of the oscillatory zone we present a…

PhysicsLeading edgeSmall dispersion limitComputer Science::Information RetrievalGeneral MathematicsMathematical analysisGeneral EngineeringMathematics::Analysis of PDEsGeneral Physics and AstronomyNonlinear equationsDispersive partial differential equationShock wavesAmplitudeNonlinear Sciences::Exactly Solvable and Integrable SystemsInitial value problemWavenumberDispersive shockDispersion (water waves)Constant (mathematics)Korteweg–de Vries equationDevries equationAsymptoticsSettore MAT/07 - Fisica MatematicaNonlinear Sciences::Pattern Formation and SolitonsMathematical Physics
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On critical behaviour in generalized Kadomtsev-Petviashvili equations

2016

International audience; An asymptotic description of the formation of dispersive shock waves in solutions to the generalized Kadomtsev–Petviashvili (KP) equation is conjectured. The asymptotic description based on a multiscales expansion is given in terms of a special solution to an ordinary differential equation of the Painlevé I hierarchy. Several examples are discussed numerically to provide strong evidence for the validity of the conjecture. The numerical study of the long time behaviour of these examples indicates persistence of dispersive shock waves in solutions to the (subcritical) KP equations, while in the supercritical KP equations a blow-up occurs after the formation of the disp…

Differential equationsShock waveSpecial solutionBlow-upKadomtsev–Petviashvili equations[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]Mathematics::Analysis of PDEsFOS: Physical sciencesPainlevé equationsKadomtsev-Petviashvili equationsKadomtsev–Petviashvili equation01 natural sciences010305 fluids & plasmasShock wavesDispersive partial differential equationMathematics - Analysis of PDEs0103 physical sciencesFOS: MathematicsCritical behaviourLong-time behaviourSupercriticalDispersion (waves)0101 mathematicsKP equationSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsMathematical physicsKadomtsev-Petviashvili equationPainleve equationsConjectureNonlinear Sciences - Exactly Solvable and Integrable Systems010102 general mathematicsMathematical analysisDispersive shocks Kadomtsev–Petviashvili equations Painlevé equations Differential equations Dispersion (waves) Ordinary differential equations Shock waves Blow-up Critical behaviour Dispersive shocks Kadomtsev-Petviashvili equation KP equation Long-time behaviour Special solutions Supercritical Partial differential equationsStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Condensed Matter PhysicsDispersive shocksPartial differential equationsNonlinear Sciences::Exactly Solvable and Integrable SystemsOrdinary differential equationSpecial solutions[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Exactly Solvable and Integrable Systems (nlin.SI)Ordinary differential equationsAnalysis of PDEs (math.AP)
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