Title: Heat Transfer
1Heat Transfer
2Outline
- Introduction
- Modes of heat transfer
- Typical design problems
- Coupling of fluid flow and heat transfer
- Conduction
- Convection
- Radiation
3Introduction
- Heat transfer is the study of thermal energy
(heat) flows - Heat always flows from hot to cold
- Examples are ubiquitous
- heat flows in the body
- home heating/cooling systems
- refrigerators, ovens, other appliances
- automobiles, power plants, the sun, etc.
4Modes of Heat Transfer
- Conduction - diffusion of heat due to temperature
gradient - Convection - when heat is carried away by moving
fluid - Radiation - emission of energy by electromagnetic
waves
qconvection
qradiation
qconduction
5Typical Design Problems
- To determine
- overall heat transfer coefficient - e.g., for a
car radiator - highest (or lowest) temperature in a system -
e.g., in a gas turbine - temperature distribution (related to thermal
stress) - e.g., in the walls of a spacecraft - temperature response in time dependent
heating/cooling problems - e.g., how long does it
take to cool down a case of soda?
6Heat Transfer and Fluid Flow
- As a fluid moves, it carries heat with it -- this
is called convection - Thus, heat transfer can be tightly coupled to the
fluid flow solution - Additionally
- The rate of heat transfer is a strong function of
fluid velocity - Fluid properties may be strong functions of
temperature (e.g., air)
7Conduction Heat Transfer
- Conduction is the transfer of heat by molecular
interaction - In a gas, molecular velocity depends on
temperature - hot, energetic molecules collide with neighbors,
increasing their speed - In solids, the molecules and the lattice
structure vibrate
8Fouriers Law
- heat flux is proportional to temperature
gradient - where k thermal conductivity
- in general, k k(x,y,z,T,)
units for q are W/m2
temperature profile
heat conduction in a slab
1
hot wall
cold wall
x
9Generalized Heat Diffusion Equation
- If we perform a heat balance on a small volume of
material - we get
heat conduction in
heat conduction out
T
heat generation
rate of change of temperature
heat cond. in/out
heat generation
thermal diffusivity
10Boundary Conditions
- Heat transfer boundary conditions generally come
in three types
q 20 W/m2 specified heat flux Neumann condition
q h(Tamb-Tbody) external heat
transfer coefficient Robin condition
T 300K specified temperature Dirichlet condition
Tbody
11Conduction Example
- Compute the heat transfer through the wall of a
home
Tout 20 F
Tout 68 F
Although slight, you can see the thermal
bridging effect through the studs
2x6 stud k0.15 W/m2-K
sheetrock k0.4 W/m2-K
shingles k0.15 W/m2-K
fiberglas insulation k0.004 W/m2-K
sheathing k0.15 W/m2-K
12Convection Heat Transfer
- Convection is movement of heat with a fluid
- E.g., when cold air sweeps past a warm body, it
draws away warm air near the body and replaces it
with cold air - often, we want to know the heat transfer
coefficient, h (next page)
flow over a heated block
13Newtons Law of Cooling
q
Tbody
average heat transfer coefficient (W/m2-K)
14Heat Transfer Coefficient
- h is not a constant, but h h(DT)
- Three types of convection
- Natural convection
- fluid moves due to buoyancy
- Forced convection
- flow is induced by external means
- Boiling convection
- body is hot enough to boil liquid
Typical values of h
Thot
Tcold
4 - 4,000 W/m2-K
Tcold
80 - 75,000
Thot
Tcold
300 - 900,000
Thot
15Looking in more detail...
- Just as there is a viscous boundary layer in the
velocity distribution, there is also a thermal
boundary layer
thermal boundary layer edge
velocity boundary layer edge
y
16Nusselt Number
- Equate the heat conducted from the wall to the
same heat transfer in convective terms - Define dimensionless quantities
- Then rearrange to get
conductivity of the fluid
Nusselt number dimensionless heat transfer
coefficient
17Energy Equation
- Generalize the heat conduction equation to
include effect of fluid motion - Assumes incompressible fluid, no shear heating,
constant properties, negligible changes in
kinetic and potential energy - Can now solve for temperature distribution in
boundary layer - Then calculate h using Fouriers law
From calculated temperature distribution
18Correlations for Heat Transfer Coefficient
- As an alternative, can use correlations to obtain
h - E.g., heat transfer from a flat plate in laminar
flow - where the Prandtl number is defined as
- Typical values are
- Pr 0.01 for liquid metals
- Pr 0.7 for most gases
- Pr 6 for water at room temperature
19Convection Examples
- Developing flow in a pipe (constant wall
temperature)
T
bulk fluid temperature
heat flux from wall
x
20Convection Examples
- Natural convection (from a heated vertical plate)
T
As the fluid is warmed by the plate, its density
decreases and a buoyant force arises which
induces flow in the vertical direction. The
force is equal to
Tw
u
The dimensionless group that governs natural
convection is the Rayleigh number
gravity
21Radiation Heat Transfer
- Thermal radiation is emission of energy as
electromagnetic waves - Intensity depends on body temperature and surface
characteristics - Important mode of heat transfer at high
temperatures - Can also be important in natural convection
problems - Examples
- toaster, grill, broiler
- fireplace
- sunshine
22Surface Characteristics
q W/m2 (incident energy flux)
rq (reflected)
aq (absorbed)
translucent slab
tq (transmitted)
absorptance
transmittance
reflectance
23Black Body Radiation
- A black body
- is a model of a perfect radiator
- absorbs all energy that reaches it reflects
nothing - therefore a 1, r t 0
- The energy emitted by a black body is the
theoretical maximum - This is Stefan-Boltzmann law s is the
Stefan-Boltzmann constant (5.6697e-8 W/m2-K4)
24Real Bodies
- Real bodies will emit less radiation than a black
body - Example radiation from a small body to its
surroundings - both the body and its surroundings emit thermal
radiation - the net heat transfer will be from the hotter to
the colder
emissivity (between 0 and 1)
25When is radiation important?
- Radiation exchange is significant in high
temperature problems e.g., combustion - Radiation properties can be strong functions of
chemical composition, especially CO2, H2O - Radiation heat exchange is difficult solve
(except for simple configurations) we must rely
on computational methods
26Heat Transfer Summary
- Heat transfer is the study of thermal energy
(heat) flows - conduction
- convection
- radiation
- The fluid flow and heat transfer problems can be
tightly coupled - through the convection term in the energy
equation - when properties (r, m) are dependent on
temperature - While analytical solutions exist for some simple
problems, we must rely on computational methods
to solve most industrially relevant applications
Can I go back to sleep now?