0000000000226187

AUTHOR

Tamara Grava

showing 7 related works from this author

Shock formation in the dispersionless Kadomtsev-Petviashvili equation

2016

The dispersionless Kadomtsev-Petviashvili (dKP) equation $(u_t+uu_x)_x=u_{yy}$ is one of the simplest nonlinear wave equations describing two-dimensional shocks. To solve the dKP equation we use a coordinate transformation inspired by the method of characteristics for the one-dimensional Hopf equation $u_t+uu_x=0$. We show numerically that the solutions to the transformed equation do not develop shocks. This permits us to extend the dKP solution as the graph of a multivalued function beyond the critical time when the gradients blow up. This overturned solution is multivalued in a lip shape region in the $(x,y)$ plane, where the solution of the dKP equation exists in a weak sense only, and a…

Shock formationFOS: Physical sciencesGeneral Physics and AstronomyKadomtsev–Petviashvili equation01 natural sciencesCritical point (mathematics)010305 fluids & plasmasDissipative dKP equation[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]Mathematics - Analysis of PDEsMethod of characteristicsPosition (vector)[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]0101 mathematicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematical physicsMathematicsCusp (singularity)Multiscales analysisdispersionless Kadomtsev-Petviashvili equation; dissipative dKP equation; multiscales analysis; shock formationPlane (geometry)Multivalued functionApplied Mathematics010102 general mathematics[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Statistical and Nonlinear PhysicsMathematical Physics (math-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemsDispersionless Kadomtsev-Petviashvili equationDissipative systemAnalysis of PDEs (math.AP)
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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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Numerical study of the Kadomtsev–Petviashvili equation and dispersive shock waves

2018

A detailed numerical study of the long time behaviour of dispersive shock waves in solutions to the Kadomtsev-Petviashvili (KP) I equation is presented. It is shown that modulated lump solutions emerge from the dispersive shock waves. For the description of dispersive shock waves, Whitham modulation equations for KP are obtained. It is shown that the modulation equations near the soliton line are hyperbolic for the KPII equation while they are elliptic for the KPI equation leading to a focusing effect and the formation of lumps. Such a behaviour is similar to the appearance of breathers for the focusing nonlinear Schrodinger equation in the semiclassical limit.

Shock waveBreatherGeneral MathematicsGeneral Physics and AstronomySemiclassical physicsFOS: Physical sciencesPattern Formation and Solitons (nlin.PS)Kadomtsev–Petviashvili equation01 natural sciences010305 fluids & plasmassymbols.namesakeMathematics - Analysis of PDEs[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]0103 physical sciencesModulation (music)FOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mathematics - Numerical Analysis0101 mathematicsSettore MAT/07 - Fisica MatematicaNonlinear Schrödinger equationNonlinear Sciences::Pattern Formation and SolitonsLine (formation)PhysicsKadomtsev-Petviashvili equationKadomtsev Petviashvili equatuonNonlinear Sciences - Exactly Solvable and Integrable SystemsDispersive Shock waves010102 general mathematicsGeneral EngineeringNumerical Analysis (math.NA)Dispersive shock waves[ MATH.MATH-NA ] Mathematics [math]/Numerical Analysis [math.NA]Whitham equationsNonlinear Sciences - Pattern Formation and SolitonsLumpsKadomtsev Petviashvili equation dispersive shock wavesClassical mechanicsNonlinear Sciences::Exactly Solvable and Integrable SystemssymbolsSolitonExactly Solvable and Integrable Systems (nlin.SI)[MATH.MATH-NA]Mathematics [math]/Numerical Analysis [math.NA]Kadomtsev Petviashvili equationAnalysis of PDEs (math.AP)
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A numerical study of the small dispersion limit of the Korteweg-de Vries equation and asymptotic solutions

2012

Abstract We study numerically the small dispersion limit for the Korteweg–de Vries (KdV) equation u t + 6 u u x + ϵ 2 u x x x = 0 for ϵ ≪ 1 and give a quantitative comparison of the numerical solution with various asymptotic formulae for small ϵ in the whole ( x , t ) -plane. The matching of the asymptotic solutions is studied numerically.

Nonlinear Sciences - Exactly Solvable and Integrable SystemsNumerical analysis010102 general mathematicsMathematical analysisMathematics::Analysis of PDEsFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Condensed Matter Physics01 natural sciences010101 applied mathematicsMathematics - Analysis of PDEsNonlinear Sciences::Exactly Solvable and Integrable SystemsFOS: MathematicsLimit (mathematics)Exactly Solvable and Integrable Systems (nlin.SI)0101 mathematicsDispersion (water waves)Korteweg–de Vries equationSettore MAT/07 - Fisica MatematicaNonlinear Sciences::Pattern Formation and SolitonsMathematical PhysicsAnalysis of PDEs (math.AP)MathematicsMathematical physicsPhys. D 241 (2012), no. 23-24, 2246–2264
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On critical behaviour in systems of Hamiltonian partial differential equations

2013

Abstract We study the critical behaviour of solutions to weakly dispersive Hamiltonian systems considered as perturbations of elliptic and hyperbolic systems of hydrodynamic type with two components. We argue that near the critical point of gradient catastrophe of the dispersionless system, the solutions to a suitable initial value problem for the perturbed equations are approximately described by particular solutions to the Painlevé-I (P $$_I$$ I ) equation or its fourth-order analogue P $$_I^2$$ I 2 . As concrete examples, we discuss nonlinear Schrödinger equations in the semiclassical limit. A numerical study of these cases provides strong evidence in support of the conjecture.

Hamiltonian PDEsFOS: Physical sciencesSemiclassical physicsPainlevé equationsArticleSchrödinger equationHamiltonian systemsymbols.namesakeMathematics - Analysis of PDEs37K05Modelling and SimulationGradient catastrophe and elliptic umbilic catastrophe34M55FOS: MathematicsInitial value problemSettore MAT/07 - Fisica MatematicaEngineering(all)Mathematical PhysicsMathematicsG100Partial differential equationConjectureNonlinear Sciences - Exactly Solvable and Integrable SystemsHyperbolic and Elliptic systemsApplied MathematicsMathematical analysisQuasi-integrable systemsGeneral EngineeringMathematical Physics (math-ph)35Q55Nonlinear systemModeling and SimulationsymbolsExactly Solvable and Integrable Systems (nlin.SI)Hamiltonian (quantum mechanics)Gradient catastrophe and elliptic umbilic catastrophe; Hamiltonian PDEs; Hyperbolic and Elliptic systems; Painlevé equations; Quasi-integrable systemsAnalysis of PDEs (math.AP)
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On universality of critical behavior in the focusing nonlinear Schrödinger equation, elliptic umbilic catastrophe and the Tritronquée solution to the…

2008

We argue that the critical behavior near the point of “gradient catastrophe” of the solution to the Cauchy problem for the focusing nonlinear Schrodinger equation \(i\epsilon \varPsi _{t}+\frac{\epsilon^{2}}{2}\varPsi _{xx}+|\varPsi |^{2}\varPsi =0\) , e ≪1, with analytic initial data of the form \(\varPsi (x,0;\epsilon)=A(x)e^{\frac{i}{\epsilon}S(x)}\) is approximately described by a particular solution to the Painleve-I equation.

Painleve equationsApplied Mathematics010102 general mathematicsGeneral EngineeringGradient catastrophe01 natural sciencesUniversality (dynamical systems)Method of undetermined coefficientsNonlinear Schrodinger equation; Gradient catastrophe; Painleve equationssymbols.namesakeModeling and SimulationModelling and Simulation0103 physical sciencessymbolsInitial value problem0101 mathematics010306 general physicsNonlinear Schrodinger equationNonlinear Schrödinger equationSettore MAT/07 - Fisica MatematicaEngineering(all)MathematicsMathematical physics
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