Introduction and basic concept. Heat Transfer

Chapter 1
INTRODUCTION AND BASIC
CONCEPTS
Copyright © 2011 The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Heat and Mass Transfer: Fundamentals & Applications
Fourth Edition
Yunus A. Cengel, Afshin J. Ghajar
McGraw-Hill, 2011
Mehmet Kanoglu
University of Gaziantep

2
Objectives
• Understand how thermodynamics and heat transfer are related
to each other
• Distinguish thermal energy from other forms of energy, and heat
transfer from other forms of energy transfer
• Perform general energy balances as well as surface energy
balances
• Understand the basic mechanisms of heat transfer, which are
conduction, convection, and radiation, and Fourier's law of heat
conduction, Newton's law of cooling, and the Stefan–Boltzmann
law of radiation
• Identify the mechanisms of heat transfer that occur
simultaneously in practice
• Develop an awareness of the cost associated with heat losses
• Solve various heat transfer problems encountered in practice

3
THERMODYNAMICS AND HEAT TRANSFER
• Heat: The form of energy that can be transferred from one
system to another as a result of temperature difference.
• Thermodynamics is concerned with the amount of heat
transfer as a system undergoes a process from one
equilibrium state to another.
• Heat Transfer deals with the determination of the rates of
such energy transfers as well as variation of temperature.
• The transfer of energy as heat is always from the higher-
temperature medium to the lower-temperature one.
• Heat transfer stops when the two mediums reach the same
temperature.
• Heat can be transferred in three different modes:
conduction, convection, radiation

5
Application Areas of Heat Transfer
5

6
Historical Background Kinetic theory: Treats molecules as
tiny balls that are in motion and thus
possess kinetic energy.
Heat: The energy associated with the
random motion of atoms and
molecules.
Caloric theory: Heat is a fluidlike
substance called the caloric that is a
massless, colorless, odorless, and
tasteless substance that can be
poured from one body into another
It was only in the middle of the
nineteenth century that we had a true
physical understanding of the nature of
heat.
Careful experiments of the Englishman
James P. Joule published in 1843
convinced the skeptics that heat was
not a substance after all, and thus put
the caloric theory to rest.

8
ENGINEERING HEAT TRANSFER
Heat transfer equipment such as heat exchangers, boilers, condensers, radiators,
heaters, furnaces, refrigerators, and solar collectors are designed primarily on the
basis of heat transfer analysis.
The heat transfer problems encountered in practice can be considered in two
groups: (1) rating and (2) sizing problems.
The rating problems deal with the determination of the heat transfer rate for an
existing system at a specified temperature difference.
The sizing problems deal with the determination of the size of a system in order to
transfer heat at a specified rate for a specified temperature difference.
An engineering device or process can be studied either experimentally (testing and
taking measurements) or analytically (by analysis or calculations).
The experimental approach has the advantage that we deal with the actual physical
system, and the desired quantity is determined by measurement, within the limits of
experimental error. However, this approach is expensive, timeconsuming, and often
impractical.
The analytical approach (including the numerical approach) has the advantage that it
is fast and inexpensive, but the results obtained are subject to the accuracy of the
assumptions, approximations, and idealizations made in the analysis.

10
• Energy can exist in numerous forms such as:
 thermal,
 mechanical,
 kinetic,
 potential,
 electrical,
 magnetic,
 chemical,
 nuclear.
• Their sum constitutes the total energy E (or e on a unit
mass basis) of a system.
• The sum of all microscopic forms of energy is called the
internal energy of a system.
HEAT AND OTHER FORMS OF ENERGY

11
• Internal energy: May be viewed as the sum of the kinetic and
potential energies of the molecules.
• Sensible heat: The kinetic energy of the molecules.
• Latent heat: The internal energy associated with the phase of a
system.
• Chemical (bond) energy: The internal energy associated with
the atomic bonds in a molecule.
• Nuclear energy: The internal energy associated with the bonds
within the nucleus of the atom itself.
What is thermal energy?
What is the difference between thermal
energy and heat?

12
Internal Energy and Enthalpy
• In the analysis of systems
that involve fluid flow, we
frequently encounter the
combination of properties u
and Pv.
• The combination is defined
as enthalpy (h = u + Pv).
• The term Pv represents the
flow energy of the fluid (also
called the flow work).

13
Specific Heats of Gases, Liquids, and Solids
• Specific heat: The energy required to raise
the temperature of a unit mass of a
substance by one degree.
• Two kinds of specific heats:
 specific heat at constant volume cv
 specific heat at constant pressure cp
• The specific heats of a substance, in
general, depend on two independent
properties such as temperature and
pressure.
• At low pressures all real gases approach
ideal gas behavior, and therefore their
specific heats depend on temperature only.

14
• Incompressible substance: A
substance whose specific volume (or
density) does not change with
temperature or pressure.
• The constant-volume and constant-
pressure specific heats are identical
for incompressible substances.
• The specific heats of incompressible
substances depend on temperature
only.

15
Energy Transfer
Energy can be transferred to or from a given
mass by two mechanisms:
heat transfer and work.
Heat transfer rate: The amount of heat
transferred per unit time.
Heat flux: The rate of heat transfer per unit
area normal to the direction of heat transfer.
when is constant:
Power: The work
done per unit time.

16
THE FIRST LAW OF THERMODYNAMICS
The energy balance for any
system undergoing any process
in the rate form
The first law of thermodynamics (conservation of energy
principle) states that energy can neither be created nor destroyed
during a process; it can only change forms.
The net change (increase or
decrease) in the total energy of
the system during a process is
equal to the difference between
the total energy entering and the
total energy leaving the system
during that process.

17
In heat transfer problems it is convenient to
write a heat balance and to treat the
conversion of nuclear, chemical,
mechanical, and electrical energies into
thermal energy as heat generation.

18
Energy Balance for Closed Systems (Fixed Mass)
A closed system consists of a fixed mass.
The total energy E for most systems
encountered in practice consists of the
internal energy U.
This is especially the case for stationary
systems since they don’t involve any
changes in their velocity or elevation during
a process.

19
Energy Balance for
Steady-Flow Systems
A large number of engineering devices such as
water heaters and car radiators involve mass flow
in and out of a system, and are modeled as
control volumes.
Most control volumes are analyzed under steady
operating conditions.
The term steady means no change with time at a
specified location.
Mass flow rate: The amount of mass flowing
through a cross section of a flow device per unit
time.
Volume flow rate: The volume of a fluid flowing
through a pipe or duct per unit time.

20
Surface Energy Balance
This relation is valid for both steady and
transient conditions, and the surface
energy balance does not involve heat
generation since a surface does not
have a volume.
A surface contains no volume or mass,
and thus no energy. Thereore, a surface
can be viewed as a fictitious system
whose energy content remains constant
during a process.

21
HEAT TRANSFER MECHANISMS
• Heat as the form of energy that can be transferred from one system to
another as a result of temperature difference.
• A thermodynamic analysis is concerned with the amount of heat
transfer as a system undergoes a process from one equilibrium state to
another.
• The science that deals with the determination of the rates of such
energy transfers is the heat transfer.
• The transfer of energy as heat is always from the higher-temperature
medium to the lower-temperature one, and heat transfer stops when
the two mediums reach the same temperature.
• Heat can be transferred in three basic modes:
 conduction
 convection
 radiation
• All modes of heat transfer require the existence of a temperature
difference.

22
Heat conduction
through a large plane
wall of thickness x
and area A.
CONDUCTION
Conduction: The transfer of energy from the more
energetic particles of a substance to the adjacent less
energetic ones as a result of interactions between the
particles.
In gases and liquids, conduction is due to the
collisions and diffusion of the molecules during their
random motion.
In solids, it is due to the combination of vibrations of
the molecules in a lattice and the energy transport by
free electrons.
The rate of heat conduction through a plane layer is
proportional to the temperature difference across the
layer and the heat transfer area, but is inversely
proportional to the thickness of the layer.

23
When x → 0 Fourier’s law of
heat conduction
Thermal conductivity, k: A measure of the ability
of a material to conduct heat.
Temperature gradient dT/dx: The slope of the
temperature curve on a T-x diagram.
Heat is conducted in the direction of decreasing
temperature, and the temperature gradient becomes
negative when temperature decreases with
increasing x. The negative sign in the equation
ensures that heat transfer in the positive x direction
is a positive quantity.
The rate of heat conduction
through a solid is directly
proportional to its thermal
conductivity.
In heat conduction
analysis, A represents
the area normal to the
direction of heat
transfer.

25
Thermal
Conductivity
Thermal conductivity:
The rate of heat transfer
through a unit thickness
of the material per unit
area per unit
temperature difference.
The thermal conductivity
of a material is a
measure of the ability of
the material to conduct
heat.
A high value for thermal
conductivity indicates
that the material is a
good heat conductor,
and a low value indicates
that the material is a
poor heat conductor or
insulator.
A simple experimental setup
to determine the thermal
conductivity of a material.

26
The range of
thermal
conductivity of
various
materials at
room
temperature.

27
The mechanisms of heat
conduction in different
phases of a substance.
The thermal conductivities of gases such
as air vary by a factor of 104
from those of
pure metals such as copper.
Pure crystals and metals have the highest
thermal conductivities, and gases and
insulating materials the lowest.

28
The variation of
the thermal
conductivity of
various solids,
liquids, and gases
with temperature.

29
Thermal Diffusivity
cp Specific heat, J/kg · °C: Heat capacity
per unit mass
cp Heat capacity, J/m3
·°C: Heat capacity
per unit volume
 Thermal diffusivity, m2
/s: Represents
how fast heat diffuses through a material
A material that has a high thermal
conductivity or a low heat capacity will
obviously have a large thermal diffusivity.
The larger the thermal diffusivity, the faster
the propagation of heat into the medium.
A small value of thermal diffusivity means
that heat is mostly absorbed by the
material and a small amount of heat is
conducted further.

30
CONVECTION
Convection: The mode of
energy transfer between a
solid surface and the
adjacent liquid or gas that is
in motion, and it involves
the combined effects of
conduction and fluid motion.
The faster the fluid motion,
the greater the convection
heat transfer.
In the absence of any bulk
fluid motion, heat transfer
between a solid surface and
the adjacent fluid is by pure
conduction.
Heat transfer from a hot surface to air
by convection.

31
Forced convection: If
the fluid is forced to flow
over the surface by
external means such as
a fan, pump, or the wind.
Natural (or free)
convection: If the fluid
motion is caused by
buoyancy forces that are
induced by density
differences due to the
variation of temperature
in the fluid.
The cooling of a boiled egg by
forced and natural convection.
Heat transfer processes that involve change of phase of a fluid are also
considered to be convection because of the fluid motion induced during
the process, such as the rise of the vapor bubbles during boiling or the
fall of the liquid droplets during condensation.

32
Newton’s law of cooling
h convection heat transfer coefficient, W/m2
· °C
As the surface area through which convection heat transfer takes place
Ts the surface temperature
T the temperature of the fluid sufficiently far from the surface.
The convection heat transfer
coefficient h is not a
property of the fluid.
It is an experimentally
determined parameter
whose value depends on all
the variables influencing
convection such as
- the surface geometry
- the nature of fluid motion
- the properties of the fluid
- the bulk fluid velocity

34
RADIATION
• Radiation: The energy emitted by matter in the form of electromagnetic
waves (or photons) as a result of the changes in the electronic
configurations of the atoms or molecules.
• Unlike conduction and convection, the transfer of heat by radiation does
not require the presence of an intervening medium.
• In fact, heat transfer by radiation is fastest (at the speed of light) and it
suffers no attenuation in a vacuum. This is how the energy of the sun
reaches the earth.
• In heat transfer studies we are interested in thermal radiation, which is
the form of radiation emitted by bodies because of their temperature.
• All bodies at a temperature above absolute zero emit thermal radiation.
• Radiation is a volumetric phenomenon, and all solids, liquids, and
gases emit, absorb, or transmit radiation to varying degrees.
• However, radiation is usually considered to be a surface phenomenon
for solids.

35
Stefan–Boltzmann law
 = 5.670  108
W/m2
· K4
Stefan–Boltzmann constant
Blackbody: The idealized surface that emits radiation at the maximum rate.
Blackbody radiation represents the maximum
amount of radiation that can be emitted from
a surface at a specified temperature.
Emissivity  : A measure of how closely
a surface approximates a blackbody for
which  = 1 of the surface. 0   1.
Radiation emitted
by real surfaces

36
Absorptivity : The fraction of the radiation energy incident on a
surface that is absorbed by the surface. 0   1
A blackbody absorbs the entire radiation incident on it ( = 1).
Kirchhoff’s law: The emissivity and the absorptivity of a surface at
a given temperature and wavelength are equal.
The absorption of radiation incident on
an opaque surface of absorptivity .

37
Radiation heat transfer between a surface
and the surfaces surrounding it.
Net radiation heat transfer:
The difference between the
rates of radiation emitted by the
surface and the radiation
absorbed.
The determination of the net
rate of heat transfer by radiation
between two surfaces is a
complicated matter since it
depends on
• the properties of the surfaces
• their orientation relative to
each other
• the interaction of the medium
between the surfaces with
radiation
Radiation is usually
significant relative to
conduction or natural
convection, but
negligible relative to
forced convection.
When a surface is completely enclosed by a
much larger (or black) surface at temperature
Tsurr separated by a gas (such as air) that
does not intervene with radiation, the net rate
of radiation heat transfer between these
two surfaces is given by

38
Combined heat transfer coefficient hcombined
Includes the effects of both convection and radiation
When radiation and convection occur
simultaneously between a surface and a gas:

39
SIMULTANEOUS HEAT
TRANSFER MECHANISMS
Although there are three mechanisms
of heat transfer, a medium may involve
only two of them simultaneously.
Heat transfer is only by conduction in opaque solids,
but by conduction and radiation in semitransparent
solids.
A solid may involve conduction and radiation but not
convection. A solid may involve convection and/or
radiation on its surfaces exposed to a fluid or other
surfaces.
Heat transfer is by conduction and possibly by
radiation in a still fluid (no bulk fluid motion) and by
convection and radiation in a flowing fluid.
In the absence of radiation, heat transfer through a
fluid is either by conduction or convection, depending
on the presence of any bulk fluid motion.
Convection = Conduction + Fluid motion
Heat transfer through a vacuum is by radiation.
Most gases between two solid surfaces
do not interfere with radiation.
Liquids are usually strong absorbers of
radiation.

40
PROBLEM-SOLVING TECHNIQUE
• Step 1: Problem Statement
• Step 2: Schematic
• Step 3: Assumptions and Approximations
• Step 4: Physical Laws
• Step 5: Properties
• Step 6: Calculations
• Step 7: Reasoning, Verification, and Discussion

43
EES (Engineering Equation Solver)
(Pronounced as ease): EES is a program that
solves systems of linear or nonlinear
algebraic or differential equations
numerically. It has a large library of built-in
thermodynamic property functions as well as
mathematical functions. Unlike some
software packages, EES does not solve
engineering problems; it only solves the
equations supplied by the user.
Engineering Software Packages
Thinking that a person who can use the
engineering software packages without
proper training on fundamentals can
practice engineering is like thinking that a
person who can use a wrench can work as
a car mechanic.

44
A Remark on Significant Digits
In engineering calculations, the
information given is not known to
more than a certain number of
significant digits, usually three
digits.
Consequently, the results
obtained cannot possibly be
accurate to more significant
digits.
Reporting results in more
significant digits implies greater
accuracy than exists, and it
should be avoided.
A result with more significant
digits than that of given data
falsely implies more accuracy.

45
Summary
• Thermodynamics and Heat Transfer
 Application areas of heat transfer
 Historical background
• Engineering Heat Transfer
 Modeling in engineering
• Heat and Other Forms of Energy
 Specific heats of gases, liquids, and solids
 Energy transfer
• The First Law of Thermodynamics
 Energy balance for closed systems (Fixed Mass)
 Energy balance for steady-flow systems
 Surface energy balance

46
• Heat Transfer Mechanisms
• Conduction
 Fourier’s law of heat conduction
 Thermal Conductivity
 Thermal Diffusivity
• Convection
 Newton’s law of cooling
• Radiation
 Stefan–Boltzmann law
• Simultaneous Heat Transfer Mechanisms
• Problem Solving Technique
 Engineering software packages
 Engineering Equation Solver (EES)
 A remark on significant digits

Introduction and basic concept. Heat Transfer

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