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Thermal expansion

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Title: Thermal expansion


1
Thermal expansion
  • Linear expansion
  • Most materials expand when heated. As long as the
    temperature change isn't too large, each
    dimension of an object experiences a change in
    length that is proportional to the change in
    temperature.
  • or, equivalently,
  • where L0 is the original length, and is the
    coefficient of linear expansion, which depends on
    the material.

Material ( 10-6/C) Material ( 10-6/C)
Aluminum 23 Glass 8.5
Copper 17 Iron 12
2
Thermal expansion
  • Volume expansion
  • For small temperature changes, we can find the
    new volume using
  • or, equivalently,
  • where V0 is the original volume.

3
Bimetallic strip
  • A bimetallic strip is made from two different
    metals that are bonded together. The strip is
    straight at room temperature, but it curves when
    it is heated. How does it work?
  • What is a common application of a bimetallic
    strip?

4
Bimetallic strip
  • A bimetallic strip is made from two different
    metals that are bonded together. The strip is
    straight at room temperature, but it curves when
    it is heated. How does it work?
  • The metals have equal lengths at
  • room temperature but different
  • expansion coefficients, so they have
  • different lengths when heated.
  • What is a common application of a bimetallic
    strip?
  • A bimetallic strip can be used as a switch in a
    thermostat. When the room is too cool the strip
    completes a circuit, turning on the furnace. The
    furnace goes off when the room (and the strip)
    warms up.

5
What happens to holes?
When an object is heated and expands, what
happens to any holes in the object? Do they get
larger or smaller? 1. The holes get smaller
2. The holes stay the same size 3. The holes
get larger
6
Holes expand, too
  • Holes expand as if they were filled with the
    surrounding material.
  • If you draw a circle on a disk and then heat the
    disk, the whole circle expands.
  • Removing the material inside the circle before
    heating produces the same result the hole
    expands.

7
Holes expand, too
8
Thermal Stress
  • If an object is heated or cooled and it is not
    free to expand or contract, the thermal stresses
    can be large enough to cause damage. This is why
    bridges have expansion joints (check this out
    where the BU bridge meets Comm. Ave.). Even
    sidewalks are built accounting for thermal
    expansion.
  • Materials that are subjected to thermal stress
    can age prematurely. For instance, over the life
    of a airplane the metal is subjected to thousands
    of hot/cold cycles that weaken the airplane's
    structure.
  • Another common example occurs with water, which
    expands by 10 when it freezes. If the water is
    in a container when it freezes, the ice can exert
    a lot of pressure on the container.

9
A black can and a white can
  • Two cans, one black and one white, are at room
    temperature. They are then exposed to a heat
    lamp. Which one heats up fastest? The cans are
    identical except for their surfaces.
  • 1. the black can
  • 2. the white can
  • 3. they heat up at the same rate

10
A black can and a white can
  • We've probably all noticed, by leaving black
    objects out in the sun, that they heat up
    fastest. The black can absorbs radiation more
    efficiently than does the white can, which
    reflects more of the radiation away.

11
A black can and a white can
  • The same two cans are then filled with hot water.
    Which cools down fastest?
  • 1. the black can
  • 2. the white can
  • 3. they cool down at the same rate

12
Heat transfer
  • Heat naturally flows from higher-temperature
    regions to lower-temperature regions.
  • The three basic mechanisms by which heat is
    transferred are conduction, convection, and
    radiation. We'll look at each of these
    separately, but in a given situation more than
    one mechanism might be important.

13
Conduction
  • Thermal conduction involves energy in the form of
    heat being transferred from a hot region to a
    cooler region through a material. At the hotter
    end, the atoms, molecules, and electrons vibrate
    with more energy than they do at the cooler end.
    The atoms, molecules, and electrons don't flow
    from one place to the other - the energy flows
    through the material, passed along by the
    vibrations.

14
Conduction
  • The rate at which heat is conducted along a bar
    of length L depends on the length, the
    cross-sectional area A, the temperature
    difference between the hot and cold ends, TH -
    TC, and the thermal conductivity k of the
    material.
  • The rate of energy transfer is power, so

15
Thermal conductivity
  • Metals generally have high thermal conductivities
    because of the free electrons that move around
    randomly. These are very efficient at
    transferring energy through the metal. Copper,
    for instance, has a thermal conductivity of 400
    W/(m K), compared to 0.024 W/(m K) for foam
    insulation.

16
R values
  • Insulating materials are rated in terms of their
    R values, which measures their resistance to
    conduction. The higher the R, the lower the
    conductivity.
  • In terms of the thickness, L

17
A conduction sandwich
  • A typical conduction problem involves creating a
    sandwich of two (or more) layers and determining
    the temperature at the interface(s) between the
    layers.
  • Consider a two-layer problem where one layer has
    twice the thickness and six times the thermal
    conductivity as the other layer, but the layers
    have the same area.

18
A conduction sandwich
  • To find the temperature at the interface between
    the layers (after thermal equilibrium has been
    reached) you should
  • 1. find that the unknown temperature is halfway
    between the temperature on one side and the
    temperature on the other side (T ?)
  • 2. set up a ratio where the change in temperature
    across a layer is proportional to the thickness
    of the layer (T ?)
  • 3. set up a ratio where the change in temperature
    across a layer is inversely proportional to the
    thickness of the layer (T ?)
  • 4. set the rate of heat flow through one layer
    equal to the rate of heat flow through the other
    layer (T ?)

19
A conduction sandwich
  • To find the temperature at the interface between
    the layers (after thermal equilibrium has been
    reached) you should
  • 1. find that the unknown temperature is halfway
    between the temperature on one side and the
    temperature on the other side (T 12 C)
  • 2. set up a ratio where the change in temperature
    across a layer is proportional to the thickness
    of the layer (T 8 C )
  • 3. set up a ratio where the change in temperature
    across a layer is inversely proportional to the
    thickness of the layer (T 16 C)
  • 4. set the rate of heat flow through one layer
    equal to the rate of heat flow through the other
    layer (T 18 C )

20
Convection
  • Heat transfer in fluids generally takes place via
    convection, in which flowing fluid carries heat
    from one place to another. Convection currents
    are produced by temperature differences. Hotter
    (less dense) parts of the fluid rise, while
    cooler (more dense) areas sink. Birds and gliders
    make use of upward convection currents to rise,
    and we also rely on convection to remove
    ground-level pollution.
  • Forced convection, where the fluid does not flow
    of its own accord but is pushed, is often used
    for heating (e.g., forced-air furnaces) or
    cooling (e.g., fans, automobile cooling systems).

21
Thermal radiation
  • Thermal radiation involves energy transferred via
    electromagnetic waves. Often this is infrared
    radiation, but it can also be visible light or
    radiation of higher energy.
  • Thermal radiation is relatively safe, and is not
    the dangerous nuclear radiation associated with
    nuclear bombs, etc.
  • All objects continually absorb thermal energy and
    radiate it away again. When everything is at the
    same temperature, the amount of energy received
    is equal to the amount given off and no changes
    in temperature occur. If an object emits more
    than it absorbs, though, it cools down.

22
Thermal radiation
  • For an object with a temperature T (in Kelvin)
    and a surface area A, the net rate of radiated
    energy depends strongly on temperature
  • where Tenv is the temperature of the surrounding
    environment, and the Stefan-Boltzmann constant is
  • s 5.67 x 10-8 W/m2
  • e is the emissivity. It is a measure of how
    efficiently an object absorbs and emits radiated
    energy. Highly reflective objects have
    emissivities close to zero. Black objects have
    emissivities close to 1. An object with e 1 is
    called a perfect blackbody.

23
Thermal radiation
  • The best absorbers are also the best emitters.
    Black objects heat up faster than shiny ones, but
    they cool down faster too.
  • This is exactly what we observe with our black
    can and white can, as the cans cool.

24
Newtons Law of Cooling
  • In many situations (and our cans are an example
    of this), the temperature of a hot object that is
    cooling follows an exponential decay. What does
    this tell us about what the rate at which the
    object loses energy? How does this rate of energy
    loss depend on temperature?

25
Newtons Law of Cooling
  • In many situations (and our cans are an example
    of this), the temperature of a hot object that is
    cooling follows an exponential decay. What does
    this tell us about what the rate at which the
    object loses energy? How does this rate of energy
    loss depend on temperature?
  • Exponential decay is characteristic of a rate
    that is proportional to a quantity, in this case
    the temperature difference between the object and
    the surroundings.
  • h is the heat transfer coefficient

26
Newtons Law of Cooling
  • With the rate of energy loss being proportional
    to the temperature difference, the exponential
    equation for the temperature of the object as a
    function of time is
  • ? is the decay rate, which depends on the surface
    area and emissivity.

27
Heat
  • What is heat?

28
Heat
  • Heat is energy transferred between a system and
    its surroundings because of a temperature
    difference between them.

29
Specific heat
  • The specific heat of a material is the amount of
    heat required to raise the temperature of 1 kg of
    the material by 1C.
  • The symbol for specific heat is c.
  • Heat lost or gained by an object is given by

Material c (J/(kg C)) Material c (J/(kg C))
Aluminum 900 Water (gas) 1850
Copper 385 Water (liquid) 4186
Gold 128 Water (ice) 2060
30
A change of state
  • Changes of state occur at particular
    temperatures, so the heat associated with the
    process is given by
  • Freezing or melting
  • where Lf is the latent heat of fusion
  • Boiling or condensing
  • where Lv is the latent heat of vaporization
  • For water the values are
  • Lf 333 kJ/kg
  • Lv 2256 kJ/kg
  • c 4.186 kJ/(kg C)

31
Which graph?
  • Simulation
  • Heat is being added to a sample of water at a
    constant rate. The water is initially solid,
    starts at -10C, and takes 10 seconds to reach
    0C.
  • You may find the following data helpful when
    deciding which graph is correct
  • Specific heats for water cliquid 1.0 cal/g C
    and
  • cice csteam 0.5 cal/g C Latent heats for
    water heat of fusion Lf 80 cal/g and heat of
    vaporization Lv 540 cal/g
  • Which graph shows correctly the temperature as a
    function of time for the first 120 seconds?

32
Which graph?
Which graph shows correctly the temperature as a
function of time for the first 120 seconds? 1.
Graph 1 2. Graph 2 3. Graph 3 4. Graph 4
5. Graph 5 6. None of the above
33
Ice water
  • 100 grams of ice, with a temperature of -10C, is
    added to a styrofoam cup of water. The water is
    initially at 10C, and has an unknown mass m. If
    the final temperature of the mixture is 0C, what
    is the unknown mass m? Assume that no heat is
    exchanged with the cup or with the surroundings.
  • Use these approximate values to determine your
    answer
  • Specific heat of liquid water is about 4000 J/(kg
    C) Specific heat of ice is about 2000 J/(kg C)
    Latent heat of fusion of water is about 3 x 105
    J/kg

34
Ice water
  • One possible starting point is to determine what
    happens if nothing changes phase. How much water
    at 10C does it take to bring 100 g of ice at
    -10C to 0C? (The water also ends up at 0C.)
  • You can do heat lost heat gained or the
    equivalent method
  • Plugging in numbers gives
  • Lot's of things cancel and we're left with
  • 100 g 2m, so m 50 g. So, that's one possible
    answer.

35
Ice water
  • Challenge for next time find the range of
    possible answers for m, the mass of the water.

36
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