Free Convection in Porous Media

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Free Convection in Porous Media

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Free Convection in Porous Media. Introduction. This model exemplifies the use of COMSOL Multiphysics for modeling of free convection in porous media. It shows the following COMSOL Multiphysics features: Porous media flow Multiphysics between fluid flow and heat transfer - PowerPoint PPT Presentation

Transcript of Free Convection in Porous Media

Free Convection in Porous Media

Introduction

• This model exemplifies the use of COMSOL Multiphysics for modeling of free convection in porous media.

• It shows the following COMSOL Multiphysics features:– Porous media flow– Multiphysics between fluid flow and heat transfer– Results that are in excellent agreement with published models in the research

journals in the field

• The model has applications mainly in the fields of:– Geophysics– Chemical engineering

Geometry, Heating and Cooling Surfaces

• Enclosed domain with porous material

• The walls of the domain are impervious to flow

• The walls are either heating or cooling surfaces with linear temperature profiles uniting the cool and hot surfaces

• The arc length s goes from zero to 1 along a boundary segment.

Th-(Th-Tc)*s

Tc

Tc

Th

Th-(Th-Tc)*s

Domain Equations

cTT TTp

k guuu

0 u

Momentum and mass balances

Heat balance

0 uTcTk p

Boussinesq buoyant lifting term links flow and heat

Brinkman equations for porous media flow

cTT TTp

k guuu

0 u

p = pressureu = vector of directional velocities = dynamic viscosityk = permeability = fluid densityg = gravityT = thermal expansion coefficientT = temperature from heat transfer applicationTc = initial temperature

Solution technique: Parametric solver to increase T from zero to problem- specific value

Convection and conduction

0 uTCTK Le

T = temperatureKe = effective thermal conductivity of fluid and solid mediumCL = fluid volumetric heat capacity… CL= cp cp = fluid specific heat capacityu = vector of directional fluid velocities from flow application

Boundary Conditions

0u• Brinkman equations

cTT

refpp for unique solution fix pressure at a point

hTT

chh TTsTT

• Convection and conduction

no slip so velocity drops to zero at wall

Results

• Dimensionless temperature • Velocity field

Concluding Remarks

• The model is simple to define and solve in COMSOL Multiphysics

• The results give excellent agreement with published scientific papers, see M. Anwar Hossain and Mike Wilson, Natural convection flow in a fluid-saturated porous medium enclosed by non-isothermal walls with heat generation, International Journal of Thermal Sciences, Int. J. Therm. Sci. 41 (2002) 447–454.