0000000000823659

AUTHOR

Peter Lindqvist

showing 7 related works from this author

Perron's method for the porous medium equation

2016

O. Perron introduced his celebrated method for the Dirichlet problem for harmonic functions in 1923. The method produces two solution candidates for given boundary values, an upper solution and a lower solution. A central issue is then to determine when the two solutions are actually the same function. The classical result in this direction is Wiener’s resolutivity theorem: the upper and lower solutions coincide for all continuous boundary values. We discuss the resolutivity theorem and the related notions for the porous medium equation ut −∆u = 0

Dirichlet problemApplied MathematicsGeneral Mathematicsta111010102 general mathematicsMathematical analysiscomparison principlePerron methodFunction (mathematics)Primary 35K55 Secondary 35K65 35K20 31C45obstaclesPorous medium equation01 natural sciencesBoundary values010101 applied mathematicsMathematics - Analysis of PDEsHarmonic functionFOS: Mathematics0101 mathematicsPorous mediumPerron methodAnalysis of PDEs (math.AP)Mathematics
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A remark on infinite initial values for quasilinear parabolic equations

2020

Abstract We study the possibility of prescribing infinite initial values for solutions of the Evolutionary p -Laplace Equation in the fast diffusion case p > 2 . This expository note has been extracted from our previous work. When infinite values are prescribed on the whole initial surface, such solutions can exist only if the domain is a space–time cylinder.

Laplace's equationSurface (mathematics)Work (thermodynamics)Applied Mathematics010102 general mathematicsMathematical analysis01 natural sciencesParabolic partial differential equationDomain (mathematical analysis)35J92 35J62010101 applied mathematicsMathematics - Analysis of PDEsFOS: MathematicsCylinder0101 mathematicsDiffusion (business)AnalysisMathematicsAnalysis of PDEs (math.AP)
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Irregular Time Dependent Obstacles

2010

Abstract We study the obstacle problem for the Evolutionary p-Laplace Equation when the obstacle is discontinuous and does not have regularity in the time variable. Two quite different procedures yield the same solution.

Yield (engineering)Parabolic obstacle problemVariational inequalities35K55 31B15 31B05Irregular obstacleLeast solutionComputer Science::RoboticsParabolic balayageLavrentiev phenomenonMathematics - Analysis of PDEsSupersolutionp-ParabolicObstacleVariational inequalityObstacle problemFOS: MathematicsApplied mathematicsTime variablePotentialAnalysisAnalysis of PDEs (math.AP)Mathematics
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A theorem of Radò’s type for the solutions of a quasi-linear equation

2004

Laplace's equationPartial differential equationLinear differential equationDifferential equationGeneral MathematicsMathematical analysisFirst-order partial differential equationRiccati equationHeat equationUniversal differential equationMathematicsMathematical Research Letters
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The ∞-Eigenvalue Problem

1999

. The Euler‐Lagrange equation of the nonlinear Rayleigh quotient \( \left(\int_{\Omega}|\nabla u|^{p}\,dx\right) \bigg/ \left(\int_{\Omega}|u|^{p}\,dx\right)\) is \( -\div\left( |\nabla u|^{p-2}\nabla u \right)= \Lambda_{p}^{p} |u |^{p-2}u,\) where \(\Lambda_{p}^{p}\) is the minimum value of the quotient. The limit as \(p\to\infty\) of these equations is found to be \(\max \left\{ \Lambda_{\infty}-\frac{|\nabla u(x)|}{u(x)},\ \ \Delta_{\infty}u(x)\right\}=0,\) where the constant \(\Lambda_{\infty}=\lim_{p\to\infty}\Lambda_{p}\) is the reciprocal of the maximum of the distance to the boundary of the domain Ω.

Mechanical EngineeringMathematical analysisMathematics::Analysis of PDEsOmegaCombinatoricsMathematics (miscellaneous)Infinity LaplacianDomain (ring theory)Nabla symbolRayleigh quotientAnalysisEigenvalues and eigenvectorsQuotientMathematicsArchive for Rational Mechanics and Analysis
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Removability of a Level Set for Solutions of Quasilinear Equations

2005

In this paper, we study the removability of a level set for the solutions of quasilinear elliptic and parabolic equations of the second order. We show, under rather general assumptions on the coeff...

Partial differential equationDifferential equationIndependent equationApplied MathematicsMathematical analysisMathematics::Analysis of PDEsParabolic partial differential equationEuler equationssymbols.namesakeMethod of characteristicsElliptic partial differential equationsymbolsHyperbolic partial differential equationAnalysisMathematicsCommunications in Partial Differential Equations
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Notes on the p-Laplace equation

2017

2. p.

osittaisdifferentiaaliyhtälötpotentiaaliteoriaepäyhtälöt
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