Search results for "Fluid Dynamic"

showing 10 items of 1034 documents

"Table 6" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2014

Inclusive jet differential cross section dsigma/dy corrected to the lepton common fiducial region and for QED radiation effects.

Physics::Fluid DynamicsInclusiveSingle Differential Cross SectionP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringZ ProductionRapidity DependenceHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentDSIG/DYRAPJet Production
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Thermophoretic separation of a ferrofluid–water emulsion: preliminary experiments

2002

Abstract The Soret effect in an emulsion (microdroplets of hydrocarbon based ferrofluid in water) is evaluated from the separation measurements in vertical thermodiffusion column. The particle concentration in column ends is detected from the resonance frequency of LC oscillators with inductance coils mounted inside the column ends. The Soret coefficient S T of droplets is calculated from the initial part of dynamic separation curves. The measured value S T =−480 K −1 agrees qualitatively well with the calculated one found assuming the Maragoni-type transfer of liquid particles.

Physics::Fluid DynamicsInductancechemistry.chemical_classificationFerrofluidMaterials scienceHydrocarbonchemistryEmulsionParticleThermodynamicsCondensed Matter PhysicsThermophoresisElectronic Optical and Magnetic MaterialsJournal of Magnetism and Magnetic Materials
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Application of Tunable-Slip Boundary Conditions in Particle-Based Simulations

2014

Compared to macroscopic systems, fluids on the micro- and nanoscales have a larger surface-to-volume ratio, thus the boundary condition becomes crucial in determining the fluid properties. No-slip boundary condition has been applied successfully to wide ranges of macroscopic phenomena, but its validity in microscopic scale is questionable. A more realistic description is that the flow exhibits slippage at the surface, which can be characterized by a Navier slip length. We present a tunable-slip method by implementing Navier boundary condition in particle-based computer simulations (Dissipative Particle Dynamics as an example). To demonstrate the validity and versatility of our method, we ha…

Physics::Fluid DynamicsInformation retrievalColloidal particleComputer scienceDissipative particle dynamicsSlip (materials science)MechanicsBoundary value problemCouette flowMicroscopic scale
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Localized forms of the LBB condition and a posteriori estimates for incompressible media problems

2018

The inf–sup (or LBB) condition plays a crucial role in analysis of viscous flow problems and other problems related to incompressible media. In this paper, we deduce localized forms of this condition that contain a collection of local constants associated with subdomains instead of one global constant for the whole domain. Localized forms of the LBB inequality imply estimates of the distance to the set of divergence free fields. We use them and deduce fully computable bounds of the distance between approximate and exact solutions of boundary value problems arising in the theory of viscous incompressible fluids. The estimates are valid for approximations, which satisfy the incompressibility …

Physics::Fluid DynamicsLBB conditiona posteriori error estimatesincompressible viscous fluidsMathematics::Analysis of PDEs
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Estimation of the Roughness Function in Turbulent Flows Using the Slope of the Roughness

2019

In the last decades, important efforts have been made to better understand the effects of surface roughness on the mean flow. These studies have been performed investigating turbulent channel flows, turbulent boundary layers or pipe flows. The most evident effect of the roughness is the increase of the overall resistance, corresponding to a decrease of the mean streamwise velocity profile in the logarithmic region. This reduction is known as roughness function \(\varDelta U^+\) (the symbol \(^+\) represents quantities made non dimensional using the friction velocity \(u_{\tau }\), or the viscous length scale \(\nu /u_{\tau }\)).

Physics::Fluid DynamicsLength scalePhysicsLogarithmTurbulenceSurface roughnessBoundary (topology)Mean flowGeometryShear velocitySurface finish
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Mean electromotive force in turbulent shear flow.

2002

We consider the mean electromotive force in turbulent shear flow taking into account the stretching of turbulent magnetic field lines by the mean flow. The mean flow can change the properties of magnetohydrodynamics-turbulence in such a way that turbulent motions become suitable for the dynamo action. The contribution of shear to the mean electromotive force cannot be described in terms of the alpha effect. The instability of the mean field arises if shear is sufficiently strong. The growth rate of instability depends on the length scale of the mean field being higher for the field with a smaller length scale. The considered mechanism may be responsible for the generation of large-scale mag…

Physics::Fluid DynamicsLength scaleShear (sheet metal)PhysicsClassical mechanicsField (physics)TurbulencePhysics::Space PhysicsMean flowMechanicsShear flowMagnetic fieldDynamoPhysical review. E, Statistical, nonlinear, and soft matter physics
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Tortuous flow in porous media

1996

The concept of tortuosity of fluid flow in porous media is discussed. A lattice-gas cellular automaton method is applied to solve the flow of a Newtonian uncompressible fluid in a two-dimensional porous substance constructed by randomly placed rectangles of equal size and with unrestricted overlap. A clear correlation between the average tortuosity of the flow paths and the porosity of the substance has been found. \textcopyright{} 1996 The American Physical Society.

Physics::Fluid DynamicsMaterials scienceFlow (mathematics)Fluid dynamicsNewtonian fluidMechanicsEqual sizePorous mediumPorosityPhysics::Classical PhysicsTortuosityCellular automaton
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A Model for Homogenization of Solid Alloying Admixtures in an Induction Crucible Furnace

2014

The paper presents a methodology for identification of homogenization time of alloying inclusions in an induction crucible furnace. The methodology is based on the Large Eddy Simulation (LES) Euler-Lagrange calculation of inclusions and a regression model for size of the inclusions and their density. The presented regression model avoids the repeated LES calculations and, therefore, is suitable for an optimization task.

Physics::Fluid DynamicsMaterials scienceMetallurgyMaterials ChemistryMetals and AlloysPhysical and Theoretical ChemistryCondensed Matter PhysicsHomogenization (chemistry)Large eddy simulationsteel research international
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Coupled Multi-Field Continuum Methods for Porous Media Fracture

2015

The focus of the present contribution is on the numerical modelling of hydraulic fracture in fluid-saturated heterogeneous materials, which can be carried out on a macroscopic scale using extended continuum porous media theories. This accounts for the crack nucleation and propagation, deformation of the solid matrix and change in the flow of the interstitial fluid. In particular, fluid-saturated porous materials basically represent volumetrically interacting solid-fluid aggregates, which are modelled using the Theory of Porous Media. The hydraulic- or tension-induced fracture occurs in the solid matrix and is simulated using a diffusive phase-field modelling approach. This way of fracture t…

Physics::Fluid DynamicsMaterials sciencePartial differential equationContinuum (measurement)Macroscopic scaleRepresentative elementary volumeNucleationMulti fieldMechanicsFracture treatmentPorous mediumPhysics::Geophysics
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The build-up and relaxation of stresses in a glass-forming soft-sphere mixture under shear: A computer simulation study

2009

Molecular-dynamics computer simulations in conjunction with Lees-Edwards boundary conditions are used to investigate a glass-forming binary Yukawa fluid under shear. The transition from the elastic response to plastic flow is elucidated by studying the stress relaxation after switching off the shear. We find a slow stress relaxation starting from states in the elastic regime and a fast one starting from states in the plastic-flow regime. We show that these relaxation patterns are related to a different distribution of local microscopic stresses in both cases.

Physics::Fluid DynamicsMaterials scienceShear (geology)Yukawa potentialStress relaxationGeneral Physics and AstronomySoft sphereStatistical physicsMechanicsBoundary value problemPlasticityGlass formingEPL (Europhysics Letters)
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