heat transfer

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Dr. ibtihal O.Alkarim Heat transfer

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Page 1: Heat transfer

Dr. i

btiha

l O.A

lkar

imHeat transfer

Page 2: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Heat vs. Temperature

Heat is the actual energy…

Temperature is the measure of average kinetic energy of particles in

a substance.

Page 3: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Heat is NOT Temperature

Page 4: Heat transfer

Dr. i

btiha

l O.A

lkar

im

What is Heat transfer?

This is the movement of thermal energy from a substance at a higher

temperature to another at a lower temperature.

Page 5: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Heat Transfer

Heat always moves from a warmer place to a cooler place.

Hot objects in a cooler room will cool to room temperature.

Cold objects in a warmer room will heat up to room temperature.

Page 6: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Heat transferheat transfer in three method

Heat transfer

conduction

convection

radiation

Page 7: Heat transfer

Dr. i

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Heat Transfer Modes

Conduction

• transfer of heat due to random molecular or atomic motion within a material (aka diffusion)

• most important in solids

Convection

• transfer of heat between a solid surface and fluid due to combined mechanisms of a) diffusion at surface; b) bulk fluid flow within boundary layer

Radiation

• transfer of heat due to emission of electromagnetic waves, usually between surfaces separated by a gas or vacuum

Page 8: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Conduction Conduction heat transfer is the flowing of heat energy from a high-temperature object to a lower-temperature object.

Page 9: Heat transfer

Dr. i

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Conduction

When you heat a metal strip at one end, the heat travels to the other end.

As you heat the metal, the particles vibrate, these vibrations make the adjacent particles vibrate, and so on and so on, the vibrations are passed along the metal and so is the heat. We call this? Conduction

Page 10: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Metals are different

The outer electrons of metal atoms drift, and are free to move.

When the metal is heated, this ‘sea of electrons’ gain kinetics energy and transfer it throughout the metal.

Insulators, such as wood and plastic, do not have this ‘sea of electrons’ which is why they do not conduct heat as well as metals.

Page 11: Heat transfer

Dr. i

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Material Thermal conductivity k (W.m-1.K-1)

diamond 2450

Cu 385

Al 205

Brick 0.2

Glass 0.8

Body fat 0.2

Water 0.6

Wood 0.2

Styrofoam

0.01

Air 0.024

Thermal conductivity, k property of the material

kdiamond very high: perfect heat sink, e.g. for high power laser diodes

khuman low: core temp relatively constant (37 oC)

kair very low: good insulator * home insulation * woolen clothing * windows double glazing

Metals – good conductors: electrons transfer energy from hot to cold

Page 12: Heat transfer

Dr. i

btiha

l O.A

lkar

im

Why does metal feel colder than wood, if they are both at the same temperature?

Metal is a conductor, wood is an insulator. Metal conducts the heat away from your hands. Wood does not conduct the heat away from your hands as well as the metal, so the wood feels warmer than the metal.

Page 13: Heat transfer

Dr. i

btiha

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For conduction between two plane surfaces (eg heat loss through the wall of a house) the rate of heat transfer is

energy transferred

through slabQ

THTC

L

H CQ T Tk At L

dQ dTk Adt dx

Thermal conductivity k (W.m-1.K-1)

steady-state

heat current H = dQ/dt

Q QA

Page 14: Heat transfer

Dr. i

btiha

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lkar

im

Heat Transfer Modes - Conduction

Steady-state heat conduction through a plane wall:

LTTkq

LTT

dxdT

dxdTk

dxdTkq

x

x

2112 ,

constant thenconstant, if

constant

L

T1 T2

x

q (T1>T2)

k

Page 15: Heat transfer

Dr. i

btiha

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lkar

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Heat Transfer Modes - Conduction

Example: What thickness of plate glass would yield the same heat flux as 3.5 of glass-fiber insulation with the same S-S temperature difference (T1-T2) ?

Page 16: Heat transfer

Dr. i

btiha

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ConvectionConvection takes place when heated

molecules move from one place to another, taking the heat with them. Convection is

common in both the atmosphere, as well as in the oceans.

Convection is the primary way that heat moves through gases and liquids.

Page 17: Heat transfer

Dr. i

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Convection

Page 18: Heat transfer

Dr. i

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Convection

What happens to the particles in a liquid or a gas when you heat them?

The particles spread out and become less dense.

This effects fluid movement.What is a fluid?A liquid or gas.

Page 19: Heat transfer

Dr. i

btiha

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lkar

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Fluid movement

Cooler, more dense, fluids sink through warmer, less dense fluids. In effect, warmer liquids and gases rise up.

Cooler liquids and gases sink.

Page 20: Heat transfer

Dr. i

btiha

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Water movement

Hot water rises

Cooler water sinks

Convection current

Cools at the surface

Page 21: Heat transfer

Dr. i

btiha

l O.A

lkar

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Cold air sinks

Where is the freezer

compartment put in a fridge?

Freezer compartment

It is put at the top, because cool air sinks, so it cools the food on the

way down.

It is warmer at the bottom, so this warmer air

rises and a convection

current is set up.

Page 22: Heat transfer

Dr. i

btiha

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http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/heatra.html

Page 23: Heat transfer

Dr. i

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Sea & Land Breezes, Monsoons

http://sol.sci.uop.edu/~jfalward/heattransfer/heattransfer.html

35 oC 20 oC 17 oC11 oC

What is the role of heat capacity, c of water and soil?

Page 24: Heat transfer

Dr. i

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lkar

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Heat Transfer Modes - Convection

Rate equation (Newton, 1700) is known as Newton’s law of “cooling”:

where q” = heat flux normal to surface q = heat rate from or to surface As

Ts = surface temperature T = freestream fluid temperature As = surface area exposed to fluid h = convection heat transfer coefficient (W/m2-K)

)(or )( TThAqTThq sss

Fluid flow, T AsTs (>T)

q

Page 25: Heat transfer

Dr. i

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Heat Transfer Modes - Convection

The convection heat transfer coefficient (h)

• is not a material property

• is a complicated function of the many parameters that influence convection such as fluid velocity, fluid properties, and surface geometry

• is often determined by experiment rather than theory

• will be given in most HW problems until we reach Chapter 6

Page 26: Heat transfer

Dr. i

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Heat Transfer Modes - Convection

Types of Convection

• Forced convection: flow caused by an external source such as a fan, pump, or atmospheric wind

• Free (or natural) convection: flow induced by buoyancy forces such as that from a heated plate

• Phase change convection: flow and latent heat exchange associated with boiling or condensation

Page 27: Heat transfer

Dr. i

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Radiation

Page 28: Heat transfer

Dr. i

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The third method of heat transfer

How does heat energy get from the Sun to the Earth? There are no particles between

the Sun and the Earth so it CANNOT travel by conduction or by convection.

?RADIATION

Page 29: Heat transfer

Dr. i

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lkar

im

RADIATION Energy transferred by electromagnetic waves

All materials radiate thermal energy in amounts determined by their temperature, where the energy is carried by photons of light in the infrared and visible portions of the electromagnetic spectrum.

Thermal radiation wavelength ranges: IR ~ 100 - 0. 8 mVisible ~ 0.8 - 0.4 m 800 – 400 nmUV ~0.4 - 0.1 m

Page 30: Heat transfer

Dr. i

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Ludwig Boltzmann        (1844-1906)

All objects above absolute zero emit radiant energy and the rate of emission increases and the peak wavelength decreases as the temperature of object increases

Page 31: Heat transfer

Dr. i

btiha

l O.A

lkar

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Power absorbed by surface of an object

A, a

Qabs

4absabs s

dQP Aa Tdt

Ts

Absorption & Stefan-Boltzmann Law

Incident radiation (INTENSITY I - energy passing through a square metre every second Iinc = P / A Iabs = a Iinc

• Surface Area, A• Absorption coefficient, a = 0 to 1• Stefan-Boltzmann constant

σ = 5.67 x 10-8 W.m-2.K-4

Page 32: Heat transfer

Dr. i

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l O.A

lkar

im

Power radiated from the surface of an object

A, e, T Qrad

4radrad

dQP Ae Tdt

net rad absPP P

Emission & Stefan-Boltzmann Law

Pnet > 0 net heat transfer out of system

• Surface Area, A• Emissivity, e = 0 to 1• Stefan-Boltzmann constant

σ = 5.67 x 10-8 W.m-2.K-4

Page 33: Heat transfer

Dr. i

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A blackbody absorbs all the radiation incident upon it and emits the max possible radiation at all wavelengths (e = a = 1)

A graybody is a surface that absorbs a certain proportion of the energy of a blackbody, the constant being constant over the entire band of wavelengths(0 e = a < 1)

emissivity e

absorption coefficient (absorptivity) a

Stefan-Boltzmann constant = 5.6710-8 W.m-2.K-4