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Heat transfer by convection

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Heat Transfer by Convection
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Page 1: Heat transfer by convection

Heat Transfer by Convection

Page 2: Heat transfer by convection

What is Convection?

Convection is a mode of heat transfer between a solid (or liquid)

surface and its adjacent liquid or gas that is in bulk motion. It

involves combined effect of conduction and fluid motion.

Newton’s Law of Cooling

π‘„π‘π‘œπ‘›π‘£ = β„Žπ΄π‘  𝑇𝑠 βˆ’ π‘‡βˆ

β„Ž is the Convection Heat Transfer Coefficient

Page 3: Heat transfer by convection

Types of Convection

1. Forced Convection:- when the fluid is forced to flow over the surface by external means

such as a fan, pump or wind.1. Natural (or Free) Convection:

- when fluid flow is caused by buoyancy forces that are induced by density differences due to variation of temperature of the fluid.

Page 4: Heat transfer by convection

The Nusselt Number

β€’ It is a dimensionless number.

β€’ It is also known as Dimensionless Convective heat Transfer

Coefficient.

β€’ It represents the enhancement of heat transfer due to bulk fluid

motion over a surface with respect to the heat transfer by

conduction.

𝑁𝑒 =β„ŽπΏπ‘Ξ»

Page 5: Heat transfer by convection

The Flow Regimes

Page 6: Heat transfer by convection

The Reynold Number

β€’ It is a dimensionless number.

β€’ It is the ratio of Inertia Forces to the Viscous Forces in a flowing

fluid.

β€’ The value of the Reynold’s Number indicates whether the flow is

laminar or turbulent.

β€’ The value of Reynold’s Number above which the flow corresponds to

turbulent flow is called Critical Reynold’s Number.

β€’ The value of Critical Reynold’s Number depends on the geometry and

flow conditions.

β€’ Typical value of Critical Reynold’s Number over a flat plate = 5 Γ— 105

𝑅𝑒 =𝑉𝐿𝑐ν

Ξ½ is the Kinematic Viscosity of the fluid Ξ½ =πœ‡

𝜌,

Where πœ‡ is the dynamic (or shear) viscosity.

Page 7: Heat transfer by convection

The Boundary Layer

Page 8: Heat transfer by convection

The Prandtle Number

β€’ It is a dimensionless number.

β€’ It is the ratio of Momentum Diffusivity (Kinematic Viscosity) to

Thermal Diffusivity.

β€’ It is the relative thickness of velocity and thermal boundary layers.

π‘ƒπ‘Ÿ =Ξ½

𝛼=πœ‡πΆπ‘Ξ»

Page 9: Heat transfer by convection

Relationship between Dimensionless Numbers

𝑁𝑒 = πΆπ‘…π‘’π‘šπ‘ƒπ‘Ÿπ‘›

For Forced Convection over a flat plate due to flow parallel to

the plate:

𝑁𝑒 = 0.664𝑅𝑒 1 2π‘ƒπ‘Ÿ 1 3a) Laminar Flow:

𝑁𝑒 = 0.037𝑅𝑒 4 5π‘ƒπ‘Ÿ 1 3a) Turbulent Flow:

Page 10: Heat transfer by convection

Numerical Exercise

1. A flat plate is supplied with a constant heat flux of 100 [W/m2]

from bottom. The plate has 0.5m2 area and is kept in a room with

ambient temperature 20Β°C. If it has a steady state temperature of

32Β°C what is the heat transfer coefficient?

π‘ž = 100 [ π‘Š π‘š2]

π‘ž = β„Ž 𝑇𝑝 βˆ’ π‘‡π‘Ž

𝑇𝑝 = 305[𝐾]

π‘‡π‘Ž = 293[𝐾]

Page 11: Heat transfer by convection

Numerical Exercise

2. The air has the following properties at 27C: Density = 1.18

[kg.m-3], Dynamic Viscosity = 1.85X10-5 [kg.m-1.s-1], Specific

Heat capacity, 𝐢𝑝 = 1.005 [kJ.kg-1.K-1]. If the thermal conductivity

of air at that temperature is Ξ» = 0.026 [W.m-1.K-1], what is the

average Nusselt Number over a flat plate of dimension 10 cm X

10 cm when air is flowing parallel to its surface with a speed 1

[ms-1]?

𝐿𝑐 = 0.1 [π‘š]

𝑉 = 1 [ π‘š 𝑠]𝑅𝑒 =

πœŒπ‘‰πΏπ‘πœ‡

π‘ƒπ‘Ÿ =πœŒπΆπ‘Ξ»

𝑁𝑒 = 0.664𝑅𝑒12π‘ƒπ‘Ÿ

13

Page 12: Heat transfer by convection

Numerical Exercise

1. Find out the thermal resistance per unit length of a plastic

insulating tube having internal radius π‘Ÿ1 = 0.001 [π‘š] and external

radius π‘Ÿ2 = 0.0015 [π‘š]. The thermal conductivity of the plastic is

Ξ» = 0.25 [π‘Š.π‘šβˆ’1. πΎβˆ’1].

π‘Ÿ1

π‘Ÿ2

𝑄 = Ξ» 2πœ‹π‘ŸπΏπ‘‘π‘‡

π‘‘π‘Ÿ

1

2πœ‹πΏΞ»

π‘Ÿ1

π‘Ÿ2 𝑄

π‘Ÿπ‘‘π‘Ÿ =

𝑇1

𝑇2

𝑑𝑇

𝑄 =2πœ‹πΏΞ»βˆ†π‘‡

lnπ‘Ÿ2π‘Ÿ1

𝑅𝑐𝑦𝑙 =βˆ†π‘‡

𝑄=ln

π‘Ÿ2π‘Ÿ1

2πœ‹πΏΞ»


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