Transcript
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.

Newtonโ€™s Law of Cooling

๐‘„๐‘๐‘œ๐‘›๐‘ฃ = โ„Ž๐ด๐‘  ๐‘‡๐‘  โˆ’ ๐‘‡โˆ

โ„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

โ€ข It is a dimensionless number.

โ€ข It is also known as Dimensionless Convective heat Transfer

Coefficient.

โ€ข It represents the enhancement of heat transfer due to bulk fluid

motion over a surface with respect to the heat transfer by

conduction.

๐‘๐‘ข =โ„Ž๐ฟ๐‘ฮป

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The Flow Regimes

Page 6: Heat transfer by convection

The Reynold Number

โ€ข It is a dimensionless number.

โ€ข It is the ratio of Inertia Forces to the Viscous Forces in a flowing

fluid.

โ€ข The value of the Reynoldโ€™s Number indicates whether the flow is

laminar or turbulent.

โ€ข The value of Reynoldโ€™s Number above which the flow corresponds to

turbulent flow is called Critical Reynoldโ€™s Number.

โ€ข The value of Critical Reynoldโ€™s Number depends on the geometry and

flow conditions.

โ€ข Typical value of Critical Reynoldโ€™s Number over a flat plate = 5 ร— 105

๐‘…๐‘’ =๐‘‰๐ฟ๐‘ฮฝ

ฮฝ is the Kinematic Viscosity of the fluid ฮฝ =๐œ‡

๐œŒ,

Where ๐œ‡ is the dynamic (or shear) viscosity.

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The Boundary Layer

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The Prandtle Number

โ€ข It is a dimensionless number.

โ€ข It is the ratio of Momentum Diffusivity (Kinematic Viscosity) to

Thermal Diffusivity.

โ€ข It is the relative thickness of velocity and thermal boundary layers.

๐‘ƒ๐‘Ÿ =ฮฝ

๐›ผ=๐œ‡๐ถ๐‘ฮป

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Relationship between Dimensionless Numbers

๐‘๐‘ข = ๐ถ๐‘…๐‘’๐‘š๐‘ƒ๐‘Ÿ๐‘›

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

the plate:

๐‘๐‘ข = 0.664๐‘…๐‘’ 1 2๐‘ƒ๐‘Ÿ 1 3a) Laminar Flow:

๐‘๐‘ข = 0.037๐‘…๐‘’ 4 5๐‘ƒ๐‘Ÿ 1 3a) Turbulent Flow:

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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 20ยฐC. If it has a steady state temperature of

32ยฐC what is the heat transfer coefficient?

๐‘ž = 100 [ ๐‘Š ๐‘š2]

๐‘ž = โ„Ž ๐‘‡๐‘ โˆ’ ๐‘‡๐‘Ž

๐‘‡๐‘ = 305[๐พ]

๐‘‡๐‘Ž = 293[๐พ]

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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, ๐ถ๐‘ = 1.005 [kJ.kg-1.K-1]. If the thermal conductivity

of air at that temperature is ฮป = 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]?

๐ฟ๐‘ = 0.1 [๐‘š]

๐‘‰ = 1 [ ๐‘š ๐‘ ]๐‘…๐‘’ =

๐œŒ๐‘‰๐ฟ๐‘๐œ‡

๐‘ƒ๐‘Ÿ =๐œŒ๐ถ๐‘ฮป

๐‘๐‘ข = 0.664๐‘…๐‘’12๐‘ƒ๐‘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 ๐‘Ÿ1 = 0.001 [๐‘š] and external

radius ๐‘Ÿ2 = 0.0015 [๐‘š]. The thermal conductivity of the plastic is

ฮป = 0.25 [๐‘Š.๐‘šโˆ’1. ๐พโˆ’1].

๐‘Ÿ1

๐‘Ÿ2

๐‘„ = ฮป 2๐œ‹๐‘Ÿ๐ฟ๐‘‘๐‘‡

๐‘‘๐‘Ÿ

1

2๐œ‹๐ฟฮป

๐‘Ÿ1

๐‘Ÿ2 ๐‘„

๐‘Ÿ๐‘‘๐‘Ÿ =

๐‘‡1

๐‘‡2

๐‘‘๐‘‡

๐‘„ =2๐œ‹๐ฟฮปโˆ†๐‘‡

ln๐‘Ÿ2๐‘Ÿ1

๐‘…๐‘๐‘ฆ๐‘™ =โˆ†๐‘‡

๐‘„=ln

๐‘Ÿ2๐‘Ÿ1

2๐œ‹๐ฟฮป


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