Search results for "partial differential equation"

showing 10 items of 326 documents

Mappings of finite distortion: The Rickman-Picard theorem for mappings of finite lower order

2004

We show that an entire mappingf of finite distortion with finite lower order can omit at most finitely many points when the distortion function off is suitably controlled. The proof uses the recently established modulus inequalities for mappings of finite distortion [15] and comparison inequalities for the averages of the counting function. A similar technique also gives growth estimates for mappings having asymptotic values.

Distortion (mathematics)Distortion functionPure mathematicsPartial differential equationGeneral MathematicsMathematical analysisLower orderFunction (mathematics)AnalysisPicard theoremMathematicsJournal d'Analyse Mathématique
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Quasiconformal distortion on arcs

1994

Distortion (mathematics)Quasiconformal mappingExtremal lengthPartial differential equationGeneral MathematicsMathematical analysisTopologyAnalysisMathematicsJournal d'Analyse Mathématique
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Optimal Shape Design in Contact Problems

1989

From the mathematical point of view, optimal shape design (or optimum design, optimization of the domain, structural optimization) is a branch of the calculus of variations and especially of optimal control where study is devoted to the problem of finding the optimal shape for an object. In an optimal shape design process the objective is to optimize certain criteria involving the solution of a partial differential equation with respect to its domain of definition, [2, 3, 5].

Domain of a functionMathematical optimizationPartial differential equationComputer scienceProcess (computing)Point (geometry)Shape optimizationOptimal controlObject (computer science)Domain (software engineering)
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Boundary accessibility and elliptic harmonic measures

1988

Suppose G is a bounded domain in R n such that the complement of G satisfies a capacity dcnsity condition. It is shown that all elliptic measures in G have a support set with Moreover, the capacity density condition cannot be removed. A nonlinear version of the result is also given.

Elliptic operatorNonlinear systemPartial differential equationBounded functionMathematical analysisBoundary (topology)Harmonic (mathematics)General MedicineDomain (mathematical analysis)Complement (set theory)MathematicsComplex Variables, Theory and Application: An International Journal
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Computational fluid dynamics and its application to transport processes

2007

Fluid transport behaviour is of great importance within the chemical process industry and in biotechnology. The complexity of this behaviour, reflected in the nature of the fundamental partial differential equations which describe it analytically, means that it has to be treated by numerical methods. In this paper the basic equations are given, and the approaches necessary to treat laminar and turbulent flows are carefully explained. As digital computers have increased in size, so has the comprehensiveness of the problems which can be treated, and the development of typical computer programs is described. Problems of accuracy and experimental validation are also surveyed, and it is shown th…

EngineeringPartial differential equationRenewable Energy Sustainability and the EnvironmentTurbulencebusiness.industryGeneral Chemical EngineeringNumerical analysisOrganic ChemistryMechanical engineeringLaminar flowComputational fluid dynamicsFluid transportPollutionInorganic ChemistryFuel TechnologyFlow (mathematics)Heat transferCFDbusinessFluid FlowWaste Management and DisposalConvective TransportBiotechnologyJournal of Chemical Technology & Biotechnology
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Nonlinear extended thermodynamics of a dilute nonviscous gas

2002

This paper deals with further developments of a nonlinear theory for a nonviscous gas in the presence of heat flux, which has been proposed in previous papers, using extended thermodynamics. The fundamental fields used are the density, the velocity, the internal energy density, and the heat flux. Using the Liu procedure, the constitutive theory is built up without approximations and the consistence of the model is showed: it is shown that the model is determined by the choice of three scalar functions which must satisfy a system of partial differential equations, which always has solutions. Different changes of field variables are carried out, using different Legendre transformations, passi…

Entropy (classical thermodynamics)Partial differential equationInternal energyHeat fluxModeling and SimulationModelling and SimulationNon-equilibrium thermodynamicsThermodynamicsThermodynamic temperatureExtended irreversible thermodynamicsAbsolute zeroMathematicsComputer Science ApplicationsMathematical and Computer Modelling
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A Fisher–Kolmogorov equation with finite speed of propagation

2010

Abstract In this paper we study a Fisher–Kolmogorov type equation with a flux limited diffusion term and we prove the existence and uniqueness of finite speed moving fronts and the existence of some explicit solutions in a particular regime of the equation.

Entropy solutionsPartial differential equationDiffusion equationApplied MathematicsMathematical analysisFlux limited diffusion equationsReaction–diffusion equationsFront propagationReaction–diffusion systemFisher–Kolmogorov equationFokker–Planck equationUniquenessDiffusion (business)Convection–diffusion equationAnalysisMathematicsJournal of Differential Equations
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Dirac equation as a quantum walk over the honeycomb and triangular lattices

2018

A discrete-time Quantum Walk (QW) is essentially an operator driving the evolution of a single particle on the lattice, through local unitaries. Some QWs admit a continuum limit, leading to well-known physics partial differential equations, such as the Dirac equation. We show that these simulation results need not rely on the grid: the Dirac equation in $(2+1)$--dimensions can also be simulated, through local unitaries, on the honeycomb or the triangular lattice. The former is of interest in the study of graphene-like materials. The latter, we argue, opens the door for a generalization of the Dirac equation to arbitrary discrete surfaces.

FOS: Computer and information sciences[ INFO ] Computer Science [cs]Differential equationFOS: Physical sciencestriangulation01 natural sciences010305 fluids & plasmassymbols.namesakeHigh Energy Physics - Lattice[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Lattice (order)Mesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciences[ PHYS.PHYS.PHYS-GEN-PH ] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]unitaritysurface[INFO]Computer Science [cs]Quantum walkHexagonal latticeDirac equationcontinuum limit010306 general physicsQuantumComputingMilieux_MISCELLANEOUSlatticeMathematical physicsPhysicsQuantum PhysicsPartial differential equationCondensed Matter - Mesoscale and Nanoscale PhysicsUnitarity[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]differential equations[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Computer Science - Distributed Parallel and Cluster ComputingDirac equationsymbolsDistributed Parallel and Cluster Computing (cs.DC)Quantum Physics (quant-ph)Physical Review A
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Simple algorithms for calculation of the axial‐symmetric heat transport problem in a cylinder

2001

The approximation of axial‐symmetric heat transport problem in a cylinder is based on the finite volume method. In the classical formulation of the finite volume method it is assumed that the flux terms in the control volume are approximated with the finite difference expressions. Then in the 1‐D case the corresponding finite difference scheme for the given source function is not exact. There we propose the exact difference scheme. In 2‐D case the corresponding integrals are approximated using different quadrature formulae. This procedure allows one to reduce the heat transport problem described by a partial differential equation to an initial‐value problem for a system of two ordinary diff…

FTCS schemeFinite volume methodDifferential equationMathematical analysisFinite difference method-Parabolic partial differential equationFinite element methodModeling and SimulationQA1-939CylinderAnalysisSIMPLE algorithmMathematicsMathematicsMathematical Modelling and Analysis
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A fully adaptive wavelet algorithm for parabolic partial differential equations

2001

We present a fully adaptive numerical scheme for the resolution of parabolic equations. It is based on wavelet approximations of functions and operators. Following the numerical analysis in the case of linear equations, we derive a numerical algorithm essentially based on convolution operators that can be efficiently implemented as soon as a natural condition on the space of approximation is satisfied. The algorithm is extended to semi-linear equations with time dependent (adapted) spaces of approximation. Numerical experiments deal with the heat equation as well as the Burgers equation.

FTCS schemeNumerical AnalysisDifferential equationIndependent equationApplied MathematicsMathematical analysisMathematicsofComputing_NUMERICALANALYSISExponential integratorParabolic partial differential equationComputational MathematicsMultigrid methodAlgorithmMathematicsNumerical stabilityNumerical partial differential equationsApplied Numerical Mathematics
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