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A Multi-Scale Three-Dimensional CFD Model of a Full Loaded Cool Storage

  • Seyed Majid Sajadiye EMAIL logo , Hojjat Ahmadi , Maryam Zolfaghari , Seyed Saeid Mohtasebi , Younes Mostofi und Amir Raja
Veröffentlicht/Copyright: 10. Mai 2013
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Abstract

A multi-scale three-dimensional computational fluid dynamics (CFD) model was developed to predict airflow, heat and mass transfer in a typical full loaded cool storage. In order to reduce the computational costs, the porous media parameters of the bed of the apples inside the vented containers were extracted using a series of wind tunnel CFD simulations and then applied in the cool storage model. The model was validated against experiments by means of velocity, product temperature, and product weight loss measurements in cool storage. The errors of about 23.2 and 9.1% were achieved for velocity magnitude prediction in the cool storage and the product weight loss after 54 days of cooling in the loaded cool storage, respectively. The model over predicted the cooling rate of the products temperature; however, it showed a good trend of cooling rate. About 11°C difference was observed between the hottest and the coldest product temperatures at half cooling time by experiments that were in good agreement with the simulation results with about 10°C. This difference changes versus time of cooling and reached to about 4°C at the end of the cooling time. The product’s temperature heterogeneity was predicted 1.9°C between the 7 and 9 hours of cooling and reduced to 0.6°C at the end of the cooling. The multi-scale model was capable of predicting air velocity, product temperature, and weight loss with reasonable accuracy and was reliable enough for numerical studies on larger domain with high reduction in computational costs.

Appendix

Nomenclature
Aotube surface area of heat exchanger, m2
Asspecific area, m2 m3
awwater activity
CForchheimer drag coefficient (inertial resistance), m1
cpmaheat capacity of moist air, J kg1 °C1
Ddiffusion of water vapor in the air, m2 s1
Dhdiameter of heat exchanger tube, m
Etotal energy, J
Ghmass velocity at minimum flow area of heat exchanger, kg m2 s1
haair film mass transfer coefficient, kg m2 s1 Pa1
hhheat transfer coefficient of heat exchanger, W m–2 °C–1
hJstatic enthalpy, J kg1
hllatent heat of water at 0°C, J kg1
hmbulk product mass transfer coefficient, kg m2 s1 Pa1
hsskin mass transfer coefficient, kg m2 s1 Pa1
j, JPheat exchanger factors
JJdiffusion flux of species, kg m2 s1
transpiration rate per unit area of product surface kg s1 m2
kturbulent kinetic energy, m2 s2
keffeffective thermal conductivity of porous zone, W m1 °C1
ppressure, Pa
Prprandtle number
Psatsaturated vapor pressure, Pa
Pvavapor pressure on the surrounding air, Pa
Pvpvapor pressure on the product surface, Pa
qprate of respiratory heat generation per unit mass of product J s1 kg1
ReReynolds number
gas constant for water vapor, 461.52 J mol1 K1
RHrelative humidity
ScSchmidt number
ShSherwood number
Shvolumetric heat sources (energy source term), J m3 s1
Simomentum source term, kg m2 s2
ttime, s
Ttemperature, K
Taveoverall average of container’s temperature, K
Tavedevaverage of the absolute deviations of temperature, K
Tcvolume average temperature of a container, K
uvelocity, m s1
ui, ujmean velocity components in X-, Y-, and Z-directions, m s1
, fluctuating velocity components, m s1
ussuperficial velocity, m s1
Vhvolume of heat exchanger, m3
vminair velocity at minimum flow area of heat exchanger unit
xi, xjCartesian coordinates, m
YWmass fraction of water vapor in the moist air
αDarcy permeability, m2
γPorosity
δijKronecker delta
εturbulent dissipation rate, m2 s3
μdynamic viscosity, kg m1 s1
μtturbulent viscosity, kg m1 s1
ρbulkapple bulk density, kg m3
ρmamoist air density, kg m3
Sub- and super-scripts
ccooler (fan and heat exchanger)
ffan
hheat exchanger
i, jCartesian coordinate index
mamoist air
pproduct (apple)
satSaturation

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Published Online: 2013-05-10

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