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Heat Transfer

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Heat transfer is the study of thermal energy (heat) flows. Heat ... toaster, grill, broiler. fireplace. sunshine. Fluent Inc. * G22. Fluids Review. TRN-1998-004 ... – PowerPoint PPT presentation

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Title: Heat Transfer


1
Heat Transfer
2
Outline
  • Introduction
  • Modes of heat transfer
  • Typical design problems
  • Coupling of fluid flow and heat transfer
  • Conduction
  • Convection
  • Radiation

3
Introduction
  • 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.

4
Modes 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
5
Typical 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?

6
Heat 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)

7
Conduction 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

8
Fouriers 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
9
Generalized 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
10
Boundary 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
11
Conduction 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
12
Convection 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
13
Newtons Law of Cooling
q
Tbody
average heat transfer coefficient (W/m2-K)
14
Heat 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
15
Looking 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
16
Nusselt 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
17
Energy 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
18
Correlations 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

19
Convection Examples
  • Developing flow in a pipe (constant wall
    temperature)

T
bulk fluid temperature
heat flux from wall
x
20
Convection 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
21
Radiation 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

22
Surface Characteristics
q W/m2 (incident energy flux)
rq (reflected)
aq (absorbed)
translucent slab
tq (transmitted)
absorptance
transmittance
reflectance
23
Black 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)

24
Real 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)
25
When 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

26
Heat 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?
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