Search results for "Internal Heat Generation"

showing 5 items of 5 documents

Low-Prandtl Number Natural Convection in Volumetrically Heated Rectangular Enclosures - III. Shallow Cavity, AR=0.25

2001

Abstract Natural convection in a volumetrically heated rectangular enclosure filled with a low-Prandtl number (Pr=0.0321) fluid was studied by direct numerical two-dimensional simulation. The enclosure had isothermal side walls and adiabatic top/bottom walls. The aspect ratio was 4 and the Grashof number Gr, based on conductive maximum temperature and cavity width, ranged from 3.79 × 104 to 1.26 × 109. According to the value of Gr, different flow regimes were obtained: steady-state, periodic, and chaotic. The first instability of the steady-state solution occurred at Gr≈3×105; the resulting time-periodic flow field consisted of a central rising plume and of convection rolls, periodically ge…

Fluid Flow and Transfer ProcessesConvectionNatural convectionMaterials scienceNatural ConvectionEnclosureMechanical EngineeringPrandtl numberEnclosureGrashof numberThermodynamicsInternal Heat GenerationMechanicsCondensed Matter PhysicsNusselt numberPlumePhysics::Fluid Dynamicssymbols.namesakeCombined forced and natural convectionsymbolsCFDSettore ING-IND/19 - Impianti Nucleari
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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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Low-Prandtl Number Natural Convection in Volumetrically Heated Rectangular Enclosures - II. Square Cavity, AR=1

2001

Natural ConvectionEnclosureInternal Heat GenerationCFDSettore ING-IND/19 - Impianti Nucleari
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Low-Prandtl Number Natural Convection in Volumetrically Heated Rectangular Enclosures - I. Slender Cavity, AR=4

2000

Natural ConvectionEnclosureInternal Heat GenerationCFDSettore ING-IND/19 - Impianti Nucleari
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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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