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Oberbeck-Boussinesq approximations and geometrical confinement effects of free convection in open cavity

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Abstract

An experimental study has been conducted on the free convection in an open cavity to investigate the effect of aspect ratio from 3.33 to 0.33 and Rayleigh number from 1.5 × 106 to 9 × 109. Also, the effect of different lateral dimensions (120 mm × 120 mm and 240 mm × 240 mm) of the bottom plate for free convection is studied. The validity of Oberbeck-Boussinesq approximation is also examined using the different approaches, such as fractional deviation in thermo-physical properties of working fluid, density variation, and Busse’s parameter. The effect of aspect ratio and the Rayleigh number on the heat transfer efficiency in free convection is observed experimentally and a power law relation having the exponent of 0.30 expressed the change in the Nusselt number with Rayleigh number. The mechanism of heat transfer in different conditions is explained using the temperature distributions with respect to Rayleigh number.

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Abbreviations

Ac :

surface area (m2)

AR:

aspect ratio

Bd :

Bond number

Cp :

specific heat (kJ/kgK)

g:

gravitational acceleration (m/s2)

h:

convective heat transfer coefficient (W/m2K)

H:

height (m)

k:

thermal conductivity (W/mK)

l:

characteristic length (m)

Nu:

Nusselt number

Pr:

Prandtl number

q:

Heat flux (W)

Qb :

Busse’s Parameter

R:

Resistance (ohm)

Ra:

Rayleigh number

T:

Temperature (K)

V:

Voltage (volt)

α:

Thermal diffusivity ()

β:

Thermal expansion coefficient (1/K)

γ:

Temperature derivative of surface tension ()

ρ:

Density (kg/m3)

ν:

Kinematic viscosity (m2/s)

qc :

Root mean square value

b:

Bottom

m:

Mean

w:

Water layer

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Correspondence to Sudhakar Subudhi.

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Choudhary, R., Saini, A. & Subudhi, S. Oberbeck-Boussinesq approximations and geometrical confinement effects of free convection in open cavity. Heat Mass Transfer 55, 2095–2102 (2019). https://doi.org/10.1007/s00231-019-02563-8

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  • DOI: https://doi.org/10.1007/s00231-019-02563-8

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