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Numerical Simulation of Mixed Convection Air ow Under a Dome-Shaped Roof By: Masih Khoshab Supervisor: Dr. A.A. Dehghan

MSc_Thesis_Conclution_02

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Numerical Simulation of Mixed Convection Airflow Under

a Dome-Shaped Roof

By: Masih KhoshabSupervisor: Dr. A.A. Dehghan

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Domed Roofs

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One of the typical underground cold water storage with domed roof equipped with wind catchers (Baadgir)

Domed Roofs & underground cold water storage

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One of the typical underground cold water storage with domed roof equipped with wind catchers (Baadgir)

Domed Roofs & underground cold water storage

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• Finite-Volume Method

• Staggered Grid

• SIMPLER Algorithm

• Scheme ADI (Implicit Line-by-Line)

• Turbulence Modeling (LRN K-ω model of Wilcox)

Solution Procedure

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Validation and Verification

Concentric Isothermal SpheresNatural convection in tall cavityMixed convection in square cavity

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Buoyancy-Induced FlowBetween Two Concentric Isothermal

Spheres

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Problem Definition

Physical Model and Coordinates System

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5107.392Ra 2.17R*

510261.2Ra *R =1.78Oi

rr

Numerical & Experimental Results

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*R 2, Pr=0.72 6Ra 1 10 5 10

Effects of Rayleigh Number

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Effects of Rayleigh Number

*R 1.5, Pr=0.73 6Ra 1 10 1 10

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*R 1.2, Pr=0.73 6Ra 1 10 1 10

Effects of Rayleigh Number

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Variation of Nusselt Number with Rayleigh Number

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Natural convection in tall cavityMixed convection in square cavity

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Natural convection in tall cavity

From Peng and Davidson, J. Heat Fluid Flow 20, 172–184 (1999)

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Streamlines and Isothermal Contours

Streamline (right) and Isothermal Contours (left)

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Peng and Davidson, J. Heat Fluid Flow 20, 172–184 (1999).Cheesewright et al., HTD 60, ASME, pp. 75–81, (1986).

Profiles at Midsection and Nu Number

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Mixed convection in square cavity

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Mixed convection in square cavity

From Peng and Davidson, J. Heat Fluid Flow 20, 172–184 (1999)Blay et al., HTD 213, ASME (1992)

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Velocity Profile at Midsection

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Temperature Profile at Midsection

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Turbulence Kinetic Energy Profile at Midsection

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Dome-Shaped Roof

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Spherical Coordinates

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Effects of Grashof Number

6 10Gr=1 10 1 10 4Re=1 10

Streamline (right) and Isothermal Contours (left)

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Effects of Reynolds Number

3 4Re=5 10 5 10 6Gr=1 10Streamline (right) and Isothermal Contours (left)

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Modifications and Accomplishments

• I extended the solver for Micropolar fluid and Nanofluid flows.

• Yuri Feldman and Tim Colonius,International Journal of Heat and Mass Transfer 64, 514–525, (2013).

• Two MSc. Student.