Search results for "Boundary value problem"

showing 10 items of 551 documents

Simple absorbing layer conditions for shallow wave simulations with Smoothed Particle Hydrodynamics

2013

Abstract We study and implement a simple method, based on the Perfectly Matched Layer approach, to treat non reflecting boundary conditions with the Smoothed Particles Hydrodynamics numerical algorithm. The method is based on the concept of physical damping operating on a fictitious layer added to the computational domain. The method works for both 1D and 2D cases, but here we illustrate it in the case of 1D and 2D time dependent shallow waves propagating in a finite domain.

PhysicsEnvironmental EngineeringOcean EngineeringFluid mechanicsMechanicsFluid mechanics Boundary condition Absorbing layer Lagrangian numerical method SPH Shallow water modelDomain (mathematical analysis)Computational physicsSmoothed-particle hydrodynamicsPerfectly matched layerSimple (abstract algebra)Boundary value problemLayer (object-oriented design)Ocean Engineering
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Influence of electromagnetic boundary conditions onto the onset of dynamo action in laboratory experiments

2009

We study the onset of dynamo action of the Riga and Karlsruhe experiments with the addition of an external wall, the electro-magnetic properties of which being different from those of the fluid in motion. We consider a wall of different thickness, conductivity and permeability. We also consider the case of a ferro-fluid in motion.

PhysicsFerrofluid[PHYS.MECA.MEFL]Physics [physics]/Mechanics [physics]/Mechanics of the fluids [physics.class-ph][SDU.STU.GP]Sciences of the Universe [physics]/Earth Sciences/Geophysics [physics.geo-ph]Fluid Dynamics (physics.flu-dyn)FOS: Physical sciences[PHYS.PHYS.PHYS-GEO-PH]Physics [physics]/Physics [physics]/Geophysics [physics.geo-ph]Physics - Fluid DynamicsConductivity01 natural sciences010305 fluids & plasmas[SPI.MECA.MEFL]Engineering Sciences [physics]/Mechanics [physics.med-ph]/Fluids mechanics [physics.class-ph]Physics::GeophysicsGeophysics (physics.geo-ph)Physics - GeophysicsPhysics::Fluid DynamicsClassical mechanicsPermeability (electromagnetism)0103 physical sciencesBoundary value problem[PHYS.MECA.MEFL]Physics [physics]/Mechanics [physics]/Fluid mechanics [physics.class-ph]010306 general physicsDynamo
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Thermal field theories and shifted boundary Conditions

2014

The analytic continuation to an imaginary velocity of the canonical partition function of a thermal system expressed in a moving frame has a natural implementation in the Euclidean path-integral formulation in terms of shifted boundary conditions. The Poincare' invariance underlying a relativistic theory implies a dependence of the free-energy on the compact length L_0 and the shift xi only through the combination beta=L_0(1+xi^2)^(1/2). This in turn implies that the energy and the momentum distributions of the thermal theory are related, a fact which is encoded in a set of Ward identities among the correlators of the energy-momentum tensor. The latter have interesting applications in latti…

PhysicsField (physics)Analytic continuationLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesThermodynamic potentialMomentumFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeMoving frameQuantum mechanicsBoundary value problemTensorMathematical physics
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Casimir-Polder interaction between an accelerated two-level system and an infinite plate

2007

We investigate the Casimir-Polder interaction energy between a uniformly accelerated two-level system and an infinite plate with Dirichlet boundary conditions. Our model is a two-level atom interacting with a massless scalar field, with a uniform acceleration in a direction parallel to the plate. We consider the contributions of vacuum fluctuations and of the radiation reaction field to the atom-wall Casimir-Polder interaction, and we discuss their dependence on the acceleration of the atom. We show that, as a consequence of the noninertial motion of the two-level atom, a thermal term is present in the vacuum fluctuation contribution to the Casimir-Polder interaction. Finally we discuss the…

PhysicsField (physics)Casimir-Polder interactionInteraction energyAtomic and Molecular Physics and OpticsCasimir effectsymbols.namesakeClassical mechanicsUnruh effectQuantum Electrodynamics in accelerated framesQuantum electrodynamicsDirichlet boundary conditionPhysics::Atomic and Molecular ClusterssymbolsUnruh effectPhysics::Atomic PhysicsBoundary value problemScalar fieldQuantum fluctuation
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Relating the finite-volume spectrum and the two-and-three-particle S matrix for relativistic systems of identical scalar particles

2017

Working in relativistic quantum field theory, we derive the quantization condition satisfied by coupled two- and three-particle systems of identical scalar particles confined to a cubic spatial volume with periodicity $L$. This gives the relation between the finite-volume spectrum and the infinite-volume $\textbf 2 \to \textbf 2$, $\textbf 2 \to \textbf 3$ and $\textbf 3 \to \textbf 3$ scattering amplitudes for such theories. The result holds for relativistic systems composed of scalar particles with nonzero mass $m$, whose center of mass energy lies below the four-particle threshold, and for which the two-particle $K$ matrix has no singularities below the three-particle threshold. The quan…

PhysicsFinite volume methodNuclear Theory010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Scattering amplitudeQuantization (physics)High Energy Physics - LatticeQuantum mechanics0103 physical sciencesGravitational singularityBoundary value problemQuantum field theory010306 general physicsNuclear theoryS-matrixPhysical Review D
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The Fučík spectrum for nonlocal BVP with Sturm–Liouville boundary condition

2014

Boundary value problem of the form x''=-μx++λx-, αx(0)+(1-α)x'(0)=0, ∫01 x(s)ds=0 is considered, where μ,λ∈ R and α∈ [0,1]. The explicit formulas for the spectrum of this problem are given and the spectra for some α values are constructed. Special attention is paid to the spectrum behavior at the points close to the coordinate origin.

PhysicsFucík spectrumApplied MathematicsSturm–Liouville boundary conditionMathematical analysisSpectrum (functional analysis)lcsh:QA299.6-433Sturm–Liouville theorylcsh:AnalysisSpectral lineboundary value problemBoundary value problemAnalysisintegral conditionNonlinear Analysis: Modelling and Control
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Atoms and molecules in cavities: A method for study of spatial confinement effects

1995

A general method for solving the problems of spatially confined quantum mechanical systems is proposed. The method works within the framework of the model space approximation. In the case of atoms and molecules trapped into any-shape microscopic cavity (like molecular sieves or fullerenes), the method reduces to a simple modification of the commonly used basis-set quantum chemical calculations. The modification consists of a particular rotation and projection in the model space, leading to solutions better adapted to the boundary conditions of the spatial confinement than the functions that describe the free systems. To illustrate how this method works, it has been applied to the hydrogen a…

PhysicsFullereneAtoms in moleculesHydrogen atomCondensed Matter PhysicsSpace (mathematics)Molecular physicsAtomic and Molecular Physics and OpticsProjection (linear algebra)Quantum mechanicsBoundary value problemPhysical and Theoretical ChemistryRotation (mathematics)QuantumInternational Journal of Quantum Chemistry
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Physical model, theoretical aspects and applications of the flight of a ball in the atmosphere. Part I: Modelling of forces and torque, and theoretic…

1991

A model of the forces and the torque operating on a ball that is flying with rotation in the atmosphere of the Earth, and the resulting system of ordinary differential equations, are derived from mechanics and aerodynamics. The system of equations allows the theoretical aspects of the flight of a ball, such as the boundedness of its kinetic energy, the curvature of the orbit or the velocity function, to be investigated using certain transformations of the variables. The solutions of the corresponding ordinary or boundary value problems, computed numerically, are used to treat certain tasks in international ball games, for example, the maximum and minimum velocities of a volleyball service.

PhysicsGeneral MathematicsGeneral EngineeringKinematicsMechanicsAerodynamicsSystem of linear equationsCurvatureClassical mechanicsOrdinary differential equationTorqueAstrophysics::Earth and Planetary AstrophysicsBoundary value problemBall (mathematics)Mathematical Methods in the Applied Sciences
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Generalized Buckley–Leverett theory for two-phase flow in porous media

2011

Hysteresis and fluid entrapment pose unresolved problems for the theory of flow in porous media. A generalized macroscopic mixture theory for immiscible two-phase displacement in porous media (Hilfer 2006b Phys. Rev. E 73 016307) has introduced percolating and nonpercolating phases. It is studied here in an analytically tractable hyperbolic limit. In this limit a fractional flow formulation exists, that resembles the traditional theory. The Riemann problem is solved analytically in one dimension by the method of characteristics. Initial and boundary value problems exhibit shocks and rarefaction waves similar to the traditional Buckley-Leverett theory. However, contrary to the traditional th…

PhysicsGeneral Physics and AstronomyMechanicsPhysics::Fluid DynamicsMixture theorysymbols.namesakeRiemann problemMethod of characteristicsBuckley–Leverett equationsymbolsTwo-phase flowBoundary value problemPorous mediumDisplacement (fluid)New Journal of Physics
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Classical thermodynamics of the Heisenberg chain in a field by generalized Bethe ansatz method

1990

Abstract Using the classical action-angle variables for the continuous model, we study the thermodynamics of the classical Heisenberg chain in an applied field by a generalized Bethe ansatz approach. The crucial point consists in the derivation of a phase-shifted density of states for the excitations of the model, obtained by imposing periodic boundary conditions. In the thermodynamic limit, the free energy can be expressed in terms of the solution of a non-linear integral equation, showing the universal dependece of the variable x=(JH) 1 2 /T .

PhysicsHeisenberg modelGeneral Physics and AstronomyThermodynamicssine-Gordon equationIntegral equationBethe ansatzsymbols.namesakeThermodynamic limitsymbolsPeriodic boundary conditionsBoundary value problemHamiltonian (quantum mechanics)Mathematical physicsPhysics Letters A
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