Search results for "Arabo"

showing 10 items of 151 documents

Quasi-linear diffusion equations with gradient terms and L1 data

2004

Abstract In this article we study the following quasi-linear parabolic problem: u t − Δ u+|u| β−2 u| ∇ u| q =|u| α−2 u| ∇ u| p in Ω×]0,T[, u(x,t)=0 on ∂Ω×]0,T[, u(x,0)=u 0 (x) in Ω, where Ω is a bounded open set of R N and T>0. We prove that if α,β>1, 0⩽p u 0 ∈L 1 (Ω) .

Partial differential equationApplied MathematicsBounded functionMathematical analysisOpen setParabolic problemQuasi linearDiffusion (business)AnalysisMathematicsNonlinear Analysis: Theory, Methods & Applications
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A free boundary problem stemmed from combustion theory. Part II: Stability, instability and bifurcation results

2002

AbstractWe deal with a free boundary problem, depending on a real parameter λ, in a infinite strip in R2, providing stability, instability and bifurcation.

Partial differential equationApplied MathematicsMathematical analysisLinearizationSaddle-node bifurcationFully nonlinear elliptic and parabolic systemsBifurcation diagramFree boundary problemsInstabilityTranscritical bifurcationLinearizationFree boundary problemBifurcationStabilityBifurcationAnalysisMathematicsJournal of Mathematical Analysis and Applications
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A FAMILY OF THE SPIRAL SOLUTIONS OF THE NONLINEAR KLEIN‐GORDON EQUATION

1998

A family of the functions, intended for a construction the exact travelling wave solutions of nonlinear partial differential equations, is given. Exact solutions of the Klein‐Gordon equation with a special potential are obtained. The behavior of complex and hypercomplex solutions of the second order is presented. First Published Online: 14 Oct 2010

Partial differential equationDifferential equationFirst-order partial differential equationExact differential equation-Kadomtsev–Petviashvili equationParabolic partial differential equationsymbols.namesakeModeling and SimulationQA1-939symbolsFisher's equationHyperbolic partial differential equationMathematicsAnalysisMathematical physicsMathematicsMathematical Modelling 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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Walsh function analysis of 2-D generalized continuous systems

1990

The importance of the generalized or singular 2D continuous systems are demonstrated by showing their use in the solution of partial differential equations in two variables. A technique is presented for solving these systems in terms of Walsh functions. The method replaces the solution of a two-variable partial differential equation with the solution of a linear algebraic generalized 2D Sylvester equation. An efficient technique for the recursive solution of the latter equation is offered. All the results apply also in the usual Roesser 2D state-space case. >

Partial differential equationDifferential equationWeak solutionMathematical analysisMathematicsofComputing_NUMERICALANALYSISFirst-order partial differential equationParabolic partial differential equationComputer Science ApplicationsMethod of characteristicsControl and Systems EngineeringComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONElectrical and Electronic EngineeringSylvester equationUniversal differential equationMathematicsIEEE Transactions on Automatic Control
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Solutions of elliptic equations with a level surface parallel to the boundary: stability of the radial configuration

2016

A positive solution of a homogeneous Dirichlet boundary value problem or initial-value problems for certain elliptic or parabolic equations must be radially symmetric and monotone in the radial direction if just one of its level surfaces is parallel to the boundary of the domain. Here, for the elliptic case, we prove the stability counterpart of that result. We show that if the solution is almost constant on a surface at a fixed distance from the boundary, then the domain is almost radially symmetric, in the sense that is contained in and contains two concentric balls $${B_{{r_e}}}$$ and $${B_{{r_i}}}$$ , with the difference r e -r i (linearly) controlled by a suitable norm of the deviation…

Partial differential equationParallel surfaces overdetermined problems method of moving planes stability stationary surfaces Harnack’s inequality.General Mathematics010102 general mathematicsMathematical analysisPrimary 35B06 35J05 35J61 Secondary 35B35 35B09Concentric01 natural sciencesParabolic partial differential equationDirichlet distributionparallel surfaces; overdetermined problems; method of moving planes; stability; stationary surfaces; Harnack's inequality010101 applied mathematicssymbols.namesakeMathematics - Analysis of PDEsMonotone polygonHomogeneousSettore MAT/05 - Analisi MatematicaNorm (mathematics)FOS: MathematicssymbolsBoundary value problem0101 mathematicsAnalysisAnalysis of PDEs (math.AP)Mathematics
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Superharmonic functions are locally renormalized solutions

2011

Abstract We show that different notions of solutions to measure data problems involving p-Laplace type operators and nonnegative source measures are locally essentially equivalent. As an application we characterize singular solutions of multidimensional Riccati type partial differential equations.

Partial differential equationSubharmonic functionApplied Mathematicsta111Mathematical analysisType (model theory)Measure (mathematics)Parabolic partial differential equationPotential theoryMathematical PhysicsAnalysisMathematicsAnnales de l'Institut Henri Poincare (C) Non Linear Analysis
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Half-width plots, a simple tool to predict peak shape, reveal column kinetics and characterise chromatographic columns in liquid chromatography: Stat…

2013

Peak profiles in chromatography are characterised by their height, position, width and asymmetry; the two latter depend on the values of the left and right peak half-widths. Simple correlations have been found between the peak half-widths and the retention times. The representation of such correlations has been called half-width plots. For isocratic elution, the plots are parabolic, although often, the parabolas can be approximated to straight-lines. The plots can be obtained with the half-widths/retention time data for a set of solutes experiencing the same kinetics, eluted with a mobile phase at fixed or varying composition. When the analysed solutes experience different resistance to mas…

Peak profiles in chromatography are characterised by their height position width and asymmetry; the two latter depend on the values of the left and right peak half-widths. Simple correlations have been found between the peak half-widths and the retention times. The representation of such correlations has been called half-width plots. For isocratic elution the plots are parabolic although often the parabolas can be approximated to straight-lines. The plots can be obtained with the half-widths/retention time data for a set of solutes experiencing the same kinetics eluted with a mobile phase at fixed or varying composition. When the analysed solutes experience different resistance to mass transfer the plots will be solute dependent and should be obtained with the data for each solute eluted with mobile phases at varying composition. The half-width plots approach is a simple tool that facilitates the prediction of peak shape (width and asymmetry) with optimisation purposes reveal the interaction kinetics of solutes in different columns and characterise chromatographic columns. This work shows half-width plots for different situations in isocratic elution including the use of different flows the effect of temperature the modification of the stationary phase surface by an additive the existence of specific interactions within the column and the comparison of columns. The adaptation to gradient elution is also described. Previous knowledge on half-width plots is structured and analysed to which new results are added.Work (thermodynamics)Column characterisationmedia_common.quotation_subjectKineticsLiquid chromatographyAnalytical chemistryHalf-widthsInteraction kineticsBiochemistryAsymmetryAnalytical ChemistryPeak shapeColumn (typography)Position (vector)Mass transferPhase (matter)media_commonChromatographyElutionChemistryOrganic ChemistryGeneral MedicineModels TheoreticalKineticsPredictionChromatography LiquidJournal of Chromatography A
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Emission and null coordinates: geometrical properties and physical construction

2011

A Relativistic Positioning System is defined by four clocks (emitters) broadcasting their proper time. Then, every event reached by the signals is naturally labeled by these four times which are the emission coordinates of this event. The coordinate hypersurfaces of the emission coordinates are the future light cones based on the emitter trajectories. For this reason the emission coordinates have been also named null coordinates or light coordinates. Nevertheless, other coordinate systems used in different relativistic contexts have the own right to be named null or light coordinates. Here we analyze when one can say that a coordinate is a null coordinate and when one can say that a coordin…

PhysicsHistoryConical coordinatesParaboloidal coordinatesAstrophysics::High Energy Astrophysical PhenomenaLog-polar coordinatesProlate spheroidal coordinatesAction-angle coordinatesParabolic coordinatesComputer Science ApplicationsEducationGeneral Relativity and Quantum CosmologyClassical mechanicsOrthogonal coordinatesBipolar coordinatesJournal of Physics: Conference Series
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Parabolic equations with natural growth approximated by nonlocal equations

2017

In this paper we study several aspects related with solutions of nonlocal problems whose prototype is $$ u_t =\displaystyle \int_{\mathbb{R}^N} J(x-y) \big( u(y,t) -u(x,t) \big) \mathcal G\big( u(y,t) -u(x,t) \big) dy \qquad \mbox{ in } \, \Omega \times (0,T)\,, $$ being $ u (x,t)=0 \mbox{ in } (\mathbb{R}^N\setminus \Omega )\times (0,T)\,$ and $ u(x,0)=u_0 (x) \mbox{ in } \Omega$. We take, as the most important instance, $\mathcal G (s) \sim 1+ \frac{\mu}{2} \frac{s}{1+\mu^2 s^2 }$ with $\mu\in \mathbb{R}$ as well as $u_0 \in L^1 (\Omega)$, $J$ is a smooth symmetric function with compact support and $\Omega$ is either a bounded smooth subset of $\mathbb{R}^N$, with nonlocal Dirichlet bound…

PhysicsKernel (set theory)Applied MathematicsGeneral Mathematics010102 general mathematicsMathematics::Analysis of PDEs01 natural sciencesParabolic partial differential equationOmega010101 applied mathematicsSymmetric functionCombinatoricssymbols.namesakeMathematics - Analysis of PDEsMathematics - Analysis of PDEs; Mathematics - Analysis of PDEsBounded functionDirichlet boundary conditionsymbolsFOS: MathematicsUniqueness0101 mathematicsAnalysis of PDEs (math.AP)
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