Search results for "Hartmann number"

showing 6 items of 6 documents

Numerical and experimental MHD studies of Lead-Lithium liquid metal flows in multichannel test-section at high magnetic fields

2018

Abstract Numerical simulation and experiments have been performed at high magnetic fields (1–3T) to study the MHD assisted molten Lead-Lithium (PbLi) flow in a model test-section which has typical features of multiple parallel channel flows as foreseen in various blanket module of ITER. The characteristics Hartmann number of the presented case study is up to 1557 which is relevant to typical fusion blanket conditions. Symbols B0, a, σ, μ in the definition of Hartmann number are strength of the applied magnetic field, characteristic length scale which is half the channel width parallel to the magnetic field, electrical conductivity and dynamic viscosity of PbLi respectively. Flow distributio…

Pressure dropMaterials scienceCharacteristic lengthMechanical EngineeringLaminar flowMechanicsHartmann number01 natural sciences010305 fluids & plasmasMagnetic fieldVolumetric flow ratePhysics::Fluid DynamicsNuclear Energy and EngineeringFlow (mathematics)0103 physical sciencesGeneral Materials ScienceMagnetohydrodynamics010306 general physicsCivil and Structural EngineeringFusion Engineering and Design
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Influence of a Magnetic Field on Liquid Metal Free Convection in an Internally Heated Cubic Enclosure

2002

The buoyancy‐driven magnetohydrodynamic flow in a cubic enclosure was investigated by three‐dimensional numerical simulation. The enclosure was volumetrically heated by a uniform power density and cooled along two opposite vertical walls, all remaining walls being adiabatic. A uniform magnetic field was applied orthogonally to the gravity vector and to the temperature gradient. The Prandtl number was 0.0321 (characteristic of Pb–17Li at 300°C), the Rayleigh number was 104, and the Hartmann number was made to vary between 0 and 2×103. The steady‐state Navier–Stokes equations, in conjunction with a scalar transport equation for the fluid's enthalpy and with the Poisson equation for the electr…

PhysicsFinite volume methodNatural convectionApplied MathematicsMechanical EngineeringPrandtl numberEnclosureFree ConvectionInternal Heat GenerationMechanicsRayleigh numberMagnetohydrodynamicHartmann numberComputer Science ApplicationsPhysics::Fluid Dynamicssymbols.namesakeClassical mechanicsMechanics of MaterialssymbolsPoisson's equationConvection–diffusion equationSettore ING-IND/19 - Impianti Nucleari
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Thermal Diffusion and Particle Separation in Ferrocolloids

1999

Results of experiments on thermal diffusion in ferrocolloids are discussed in the paper. The Soret coefficient is evaluated from measurements of particle separation in thermodiffusion column. To interpret the separation curves measured in the presence of a magnetic field, the column theory is modified taking into account for MHD effects of free convection. It is shown that the Hartmann effect in hydrocarbon based colloids as well in ionic magnetic fluids does not influence significantly the particle separation dynamics. From unsteady separation curves positive values of the Soret coefficient of surfacted particles in tetradecane based colloids are calculated. Such direction of particle tran…

Physics::Fluid DynamicsTemperature gradientMaterials scienceNatural convectionParticleThermodynamicsThermal diffusivityHartmann numberHydrodynamic theoryThermophoresisMagnetic field
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Liquid metal MHD studies with non-magnetic and ferro-magnetic structural material

2014

Abstract In most of the liquid metal MHD experiments reported in the literature to study liquid breeder blanket performance, SS316/SS304 grade steels are used as the structural material which is non-magnetic. On the other hand, the structural material for fusion blanket systems has been proposed to be ferritic martensitic grade steel (FMS) which is ferromagnetic in nature. In the recent experimental campaign, liquid metal MHD experiments have been carried out with two identical test sections: one made of SS316L (non-magnetic) and another with SS430 (ferromagnetic), to compare the effect of structural materials on MHD phenomena for various magnetic fields (up to 4 T). The maximum Hartmann nu…

Pressure dropLiquid metalMaterials scienceMechanical EngineeringMechanicsBlanketHartmann numberMagnetic fieldNuclear Energy and EngineeringFerromagnetismPerpendicularGeneral Materials ScienceMagnetohydrodynamicsCivil and Structural EngineeringFusion Engineering and Design
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MHD free convection in a liquid-metal filled cubic enclosure. II. Internal heating

2002

The buoyancy-driven magnetohydrodynamic flow in a liquid-metal filled cubic enclosure was investigated by three-dimensional numerical simulation. The enclosure was differentially heated at two opposite vertical walls, all other walls being adiabatic, and a uniform magnetic field was applied orthogonal to the temperature gradient and to the gravity vector. The Rayleigh number was 105 and the Prandtl number was 0.0321 (characteristic of Pb–17Li at 573 K). The Hartmann number was made to vary between 102 and 103 and the electrical conductance of the walls between 0 and ∞. The continuity, momentum and enthalpy transport equations, in conjunction with a Poisson equation for the electric potentia…

Fluid Flow and Transfer ProcessesConvectionPhysicsNatural convectionEnclosureMechanical EngineeringPrandtl numberEnclosureFree ConvectionInternal Heat GenerationThermodynamicsRayleigh numberMechanicsMagnetohydrodynamicCondensed Matter PhysicsHartmann numberPhysics::Fluid Dynamicssymbols.namesakesymbolsMagnetohydrodynamic driveMagnetohydrodynamicsCFDSettore ING-IND/19 - Impianti NucleariInternational Journal of Heat and Mass Transfer
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3D MHD lead–lithium liquid metal flow analysis and experiments in a Test-Section of multiple rectangular bends at moderate to high Hartmann numbers

2013

Abstract Experiments with liquid lead–lithium (Pb–Li) were carried out in a stainless steel (SS) Test Section (TS) consisting of multiple 90° bends for various flow rates and applied magnetic fields of up to 4 T. Characteristic MHD flow parameter Hartmann number, Ha ( = B 0 a σ / μ , Ha2 is the ratio of electromagnetic force to viscous force) and interaction parameter, N ( = σ a B 0 2 / ρ U , N is the ratio of electromagnetic force to inertial force) of these experiments were varied from Ha = 515 to 2060 and N = 25 to 270 by changing the applied magnetic field and flow rates respectively. Three dimensional numerical simulations have been carried out using MHD module of FLUENT code. The meas…

PhysicsField (physics)Turbulencebusiness.industryMechanical EngineeringLaminar flowMechanicsHartmann numberMagnetic fieldPhysics::Fluid DynamicsOpticsNuclear Energy and EngineeringFictitious forceGeneral Materials ScienceElectric potentialMagnetohydrodynamicsbusinessCivil and Structural EngineeringFusion Engineering and Design
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