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Numerical Heat Transfer, Part A: Applications
An International Journal of Computation and Methodology
Volume 70, 2016 - Issue 7
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Original Articles

Analysis of entropy generation for mixed convection within porous square cavities: Effects of various moving walls

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Pages 738-762 | Received 23 Nov 2015, Accepted 20 Apr 2016, Published online: 18 Aug 2016
 

ABSTRACT

The aim of the present investigation is to analyze the effect of the motion of horizontal (cases 1a–1d) and vertical walls (case 2a–2c) on the entropy generation and heat transfer in a porous square cavity during mixed convection. The cavity is subject to the thermal boundary conditions such as the hot bottom wall, cold side walls, and thermally insulated top wall. Analysis has been done for various fluids with Prandtl number, Prm = 0.026–7.2, Grashof number, Gr = 105, Reynolds number, Re = 10–100, and Darcy number, Dam = 10−4–10−2. Numerical results are presented using streamfunction (ψ), local entropy generation due to fluid friction (Sψ), isotherms (θ), and local entropy generation due to heat-transfer (Sθ) contours. In addition, the total entropy generation (Stotal), average Bejan number (Beav), and overall heat-transfer rate at the hot bottom wall are analyzed and discussed.

Nomenclature

Be=

Bejan number

Dam=

modified Darcy number

g=

acceleration due to gravity, m s−2

Gr=

Grashof number

K=

medium permeability

L=

length of the square cavity, m

=

average Nusselt number

P=

dimensionless pressure

Prm=

modified Prandtl number

Re=

Reynolds number

Sθ=

dimensionless entropy generation due to heat transport

Sψ=

dimensionless entropy generation due to fluid friction

T=

temperature of the fluid, K

U=

x component of dimensionless velocity

U0=

characteristic velocity

V=

y component of dimensionless velocity

X=

dimensionless distance along x coordinate

Y=

dimensionless distance along y coordinate

α=

thermal diffusivity, m2s−1

β=

volume expansion coefficient, K−1

γ=

penalty parameter

θ=

dimensionless temperature

ρ=

density, kg m−3

Φ=

basis functions

ψ=

dimensionless streamfunction

μ=

dynamic viscosity, kg m−1 s−1

ε=

porosity of the medium

Subscripts
av=

spatial average

eff=

effective

Superscripts
e=

element

Nomenclature

Be=

Bejan number

Dam=

modified Darcy number

g=

acceleration due to gravity, m s−2

Gr=

Grashof number

K=

medium permeability

L=

length of the square cavity, m

=

average Nusselt number

P=

dimensionless pressure

Prm=

modified Prandtl number

Re=

Reynolds number

Sθ=

dimensionless entropy generation due to heat transport

Sψ=

dimensionless entropy generation due to fluid friction

T=

temperature of the fluid, K

U=

x component of dimensionless velocity

U0=

characteristic velocity

V=

y component of dimensionless velocity

X=

dimensionless distance along x coordinate

Y=

dimensionless distance along y coordinate

α=

thermal diffusivity, m2s−1

β=

volume expansion coefficient, K−1

γ=

penalty parameter

θ=

dimensionless temperature

ρ=

density, kg m−3

Φ=

basis functions

ψ=

dimensionless streamfunction

μ=

dynamic viscosity, kg m−1 s−1

ε=

porosity of the medium

Subscripts
av=

spatial average

eff=

effective

Superscripts
e=

element

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