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Numerical Heat Transfer, Part A: Applications
An International Journal of Computation and Methodology
Volume 69, 2016 - Issue 8
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Original Articles

Opposing buoyancy characteristics of Newtonian fluid flow around a confined square cylinder at low and moderate Reynolds numbers

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Pages 874-897 | Received 14 May 2015, Accepted 20 Jul 2015, Published online: 01 Feb 2016
 

ABSTRACT

The influence of opposing-buoyancy mixed convection from a square cylinder in a vertical channel has been studied at Reynolds numbers (Re) = 1–100, Richardson numbers (Ri) = 0 to −1, and blockage ratios (β) = 10–50% for air as a working fluid. The onset of a steady to a time-periodic regime is found for Ri = 0 (at Re = 35, 65, 74, and 62), Ri = −0.5 (at Re = 12, 39, 48, and 54), and Ri = −1 (at Re = 9, 30, 39, and 50) for β = 10%, 25%, 30%, and 50%, respectively. The initiation of flow separation is also determined. Finally, the correlations of Strouhal number, drag coefficient, and the Colburn heat transfer factor were obtained.

Nomenclature

CD=

total drag coefficient

CDF=

friction drag coefficient

CDp=

pressure drag coefficient

CL=

lift coefficient

Cp=

constant-pressure specific heat of the fluid (J/kgK)

d=

side of a square cylinder (m)

f=

frequency of vortex shedding (1/s)

FD=

drag force per unit object length (N/m)

FDF=

frictional force per unit object length (N/m)

FDP=

pressure force per unit object length (N/m)

FL=

lift force per unit object length (N/m)

g=

acceleration due to gravity (m/s2)

Gr=

Grashof number

h=

local convective heat transfer coefficient (W/m2K)

=

average convective heat transfer coefficient (W/m2K)

H=

computational domain height (m)

jh=

Colburn heat transfer factor

k=

thermal conductivity of the fluid (W/mK)

Nu=

local Nusselt number

=

average Nusselt number

ns=

normal direction

p=

pressure

Pr=

Prandtl number

Re=

Reynolds number

Ri=

Richardson number

St=

Strouhal number

t=

time

T=

temperature (K)

TP=

time period of one cycle

T=

fluid temperature at the inlet (K)

Tw=

surface temperature of the square cylinder (K)

u=

x-velocity component

v=

y-velocity component

V=

average velocity of fluid at the inlet (m/s)

x=

stream-wise coordinate

Xd=

downstream distance (m)

Xu=

upstream distance (m)

y=

crossways coordinate

βv=

volume expansion coefficient (1/K)

β=

blockage ratio

θ=

temperature gradient

μ=

fluid viscosity (Pa s)

ρ=

fluid density (kg/m3)

Superscript=
=

dimensional value

Nomenclature

CD=

total drag coefficient

CDF=

friction drag coefficient

CDp=

pressure drag coefficient

CL=

lift coefficient

Cp=

constant-pressure specific heat of the fluid (J/kgK)

d=

side of a square cylinder (m)

f=

frequency of vortex shedding (1/s)

FD=

drag force per unit object length (N/m)

FDF=

frictional force per unit object length (N/m)

FDP=

pressure force per unit object length (N/m)

FL=

lift force per unit object length (N/m)

g=

acceleration due to gravity (m/s2)

Gr=

Grashof number

h=

local convective heat transfer coefficient (W/m2K)

=

average convective heat transfer coefficient (W/m2K)

H=

computational domain height (m)

jh=

Colburn heat transfer factor

k=

thermal conductivity of the fluid (W/mK)

Nu=

local Nusselt number

=

average Nusselt number

ns=

normal direction

p=

pressure

Pr=

Prandtl number

Re=

Reynolds number

Ri=

Richardson number

St=

Strouhal number

t=

time

T=

temperature (K)

TP=

time period of one cycle

T=

fluid temperature at the inlet (K)

Tw=

surface temperature of the square cylinder (K)

u=

x-velocity component

v=

y-velocity component

V=

average velocity of fluid at the inlet (m/s)

x=

stream-wise coordinate

Xd=

downstream distance (m)

Xu=

upstream distance (m)

y=

crossways coordinate

βv=

volume expansion coefficient (1/K)

β=

blockage ratio

θ=

temperature gradient

μ=

fluid viscosity (Pa s)

ρ=

fluid density (kg/m3)

Superscript=
=

dimensional value

Acknowledgements

The authors would like to thank two anonymous reviewers for their positive comments on this work.

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