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    PHYS222 LSSU Bazlur Slide 1

    Chapter - 12

    Temperature

    and

    Heat

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    PHYS222 LSSU Bazlur Slide 2

    Temperature and Heat

    12.1 Common Temperature Scales

    12.2 The Kelvin Temperature Scales12.3 Thermometers

    12.4 Linear Thermal Expansion

    12.5 Volume Thermal Expansion

    12.6 Heat and Internal Energy

    12.7 Heat and Temperature Change: Specific HeatCapacity

    12.8 Heat and Phase Change: Latent Heat12.9 Equilibrium between Phases of Matter

    12.10 Humidity

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    12.1 Common Temperature Scales

    Temperatures are reported in degrees

    Celsiusor degrees Fahrenheit.

    Temperatures changed, on theother hand, are reported in Celsius

    degrees or Fahrenheitdegrees:

    F

    5

    9C1

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    12.1 Common Temperature Scales

    Example 1 Converting from a Fahrenheit to a Celsius Temperature

    A healthy person has an oral temperature of 98.6o

    F. What would thisreading be on the Celsius scale?

    F6.66F32F98.6

    degrees above ice point

    C0.37F

    C1F6.66

    59

    C0.37C0.37C0

    ice point

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    12.1 Common Temperature Scales

    Example 2 Converting from a Celsius to a Fahrenheit Temperature

    A time and temperature sign on a bank indicates that the outdoor

    temperature is -20.0oC. Find the corresponding temperature on

    the Fahrenheit scale.

    F0.36C1

    FC0.20 5

    9

    degrees below ice point

    F0.4F0.36F0.32

    ice point

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    12.2 The Kelvin Temperature Scale

    15.273 cTT

    Kelvin temperature

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    12.2 The Kelvin Temperature Scale

    A con stant-volum e gas

    thermometer.

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    12.2 The Kelvin Temperature Scale

    abso lute zero po int = -273.15oC

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    12.3 Thermometers

    Thermometers make use of the change in some physical property with temperature.

    A property that changes with temperature is called a thermometr ic prop erty.

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    12.4 Linear Thermal Expansion

    NORMAL SOLIDS

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    12.4 Linear Thermal Expansion

    oLL

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    12.4 Linear Thermal Expansion

    LINEAR THERMAL EXPANSION OF A SOLID

    The length of an object changes when its temperature changes:

    TLL o

    coefficient of

    linear expansion

    Comm on Unit for the Coeffic ient of Linear Expansion: 1CC

    1

    12 4 Li Th l E i

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    12.4 Linear Thermal Expansion

    12 4 Li Th l E i

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    12.4 Linear Thermal Expansion

    Example 3 The Buckling of a Sidewalk

    A concrete sidewalk is constructed between

    two buildings on a day when the temperature

    is 25oC. As the temperature rises to 38oC,the slabs expand, but no space is provided for

    thermal expansion. Determine the distance y

    in part (b) of the drawing.

    12 4 Li Th l E i

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    12.4 Linear Thermal Expansion

    m00047.0C13m0.3C1012 16

    TLL o

    m053.0m00000.3m00047.3 22 y

    12 4 Li Th l E i

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    12.4 Linear Thermal Expansion

    Example 4 The Stress on a Steel Beam

    The beam is mounted between two

    concrete supports when the temperature

    is 23oC. What compressional stress

    must the concrete supports apply to

    each end of the beam, if they are

    to keep the beam from expanding

    when the temperature rises to 42oC?

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    2716211 mN107.4C19C1012mN100.2

    Stress

    TYL

    LY

    A

    F

    o

    TLL o

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    THE BIMETALLIC STRIP

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    THE EXPANSION OF HOLES

    Conceptual Examp le 5The Expansion of Holes

    The figure shows eight square tiles that are arranged to form a square pattern

    with a hold in the center. If the tiled are heated, what happens to the size of the

    hole?

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    A hole in a piece of solid material expands when heated and contracts when

    cooled, just as if it were filled with the material that surrounds it.

    12 4 Linear Thermal Expansion

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    12.4 Linear Thermal Expansion

    Conceptu al Examp le 7 Expanding Cylinders

    Each cylinder is made from a different material.

    All three have the same temperature and theybarely fit inside each other.

    As the cylinders are heated to the same,

    but higher, temperature, cylinder C falls

    off, while cylinder A becomes tightly wedged

    to cylinder B.

    Which cylinder is made from which material?

    12 5 Volume Thermal Expansion

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    12.5 Volume Thermal Expansion

    VOLUME THERMAL EXPANSION

    The volume of an object changes when its temperature changes:

    TVV o

    coefficient of

    volume expansion

    Comm on Unit for the Coeffic ient of Volum e Expansion : 1CC

    1

    12 5 Volume Thermal Expansion

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    PHYS222 LSSU Bazlur Slide 25

    12.5 Volume Thermal Expansion

    Example 8 An Automobile Radiator

    A small plastic container, called the coolant reservoir, catches

    the radiator fluid that overflows when an automobile enginebecomes hot. The radiator is made of

    copper and the coolant has an

    expansion coefficient of

    4.0x10-4(Co)-1. If the radiator

    is filled to its 15-quart capacitywhen the engine is cold (6oC),

    how much overflow will spill into the

    reservoir when the coolant reaches its

    operating temperature (92oC)?

    12.5 Volume Thermal Expansion

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    12.5 Volume Thermal Expansion

    quarts53.0C86quarts15C1010.4 14coolant V

    quarts066.0C86quarts15C1051 16radiator V

    quarts0.46quarts066.0quarts53.0spill V

    12.5 Volume Thermal Expansion

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    PHYS222 LSSU Bazlur Slide 27

    12.5 Volume Thermal Expansion

    Expansion of water.

    12.6 Heat and Internal Energy

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    PHYS222 LSSU Bazlur Slide 28

    6 eat a d te a e gy

    DEFINITION OF HEAT

    Heat is energy that flows from a higher-

    temperature object to a lower-temperature

    object because of a difference in temperatures.

    SI Unit of Heat: joule (J)

    12.6 Heat and Internal Energy

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    PHYS222 LSSU Bazlur Slide 29

    gy

    The heat that flows from hot to cold

    originates in the internal energy of

    the hot substance.

    It is not correct to say that a substance

    contains heat.

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 30

    p g p p y

    SOLIDS AND LIQUIDS

    HEAT SUPPLIED OR REMOVED IN CHANGING THE TEMPERATURE

    OF A SUBSTANCE

    The heat that must be supplied or removed to change the temperature of

    a substance is

    TmcQ

    specific heat

    capacity

    Common Unit for Specific Heat Capacity: J/(kgCo)

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 31

    p g p p y

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 32

    p g p p y

    Examp le 9 A Hot Jogger

    In a half-hour, a 65-kg jogger can generate 8.0x105

    J of heat. This heatis removed from the body by a variety of means, including the bodys own

    temperature-regulating mechanisms. If the heat were not removed, how

    much would the body temperature increase?

    TmcQ

    C5.3CkgJ3500kg65

    J100.8 5

    mc

    QT

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 33

    GASES

    The value of the specific heat of a gas depends on whether the pressure or

    volume is held constant.

    This distinction is not important for solids.

    OTHER UNITS

    1 kcal = 4186 joules

    1 cal = 4.186 joules

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 34

    CALORIMETRY

    If there is no heat loss to the surroundings,

    the heat lost by the hotter object equals theheat gained by the cooler ones.

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    Example 12 Measuring the Specific Heat Capacity

    The calorimeter is made of 0.15 kg of aliminumand contains 0.20 kg of water. Initially, the

    water and cup have the same temperature

    of 18.0oC. A 0.040 kg mass of unknown

    material is heated to a temperature of

    97.0o

    C and then added to the water.

    After thermal equilibrium is reached, the

    temperature of the water, the cup, and the

    material is 22.0oC. Ignoring the small amount

    of heat gained by the thermometer, find

    the specific heat capacity of the

    unknown material.

    12.7 Heat and Temperature Change: Specific Heat Capacity

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    PHYS222 LSSU Bazlur Slide 36

    unknownwaterAl TmcTmcTmc

    CkgJ1300

    C0.75kg040.0

    C0.4kg20.0CkgJ4186C0.4kg15.0CkgJ1000.9 2

    unknown

    waterAlunknown

    Tm

    TmcTmcc

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 37

    THE PHASES OF MATTER

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 38

    During a phase change, the temperature of the mixture does not

    change (provided the system is in thermal equilibrium).

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 39

    Conceptu al Example 13 Saving Energy

    Suppose you are cooking spaghetti for dinner, and the instructions

    say boil pasta in water for 10 minutes. To cook spaghetti in an open

    pot with the least amount of energy, should you turn up the burner

    to its fullest so the water vigorously boils, or should you turn down

    the burner so the water barely boils?

    12.8 Heat and Phase Change: Latent Heat

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    HEAT SUPPLIED OR REMOVED IN CHANGING THE PHASE

    OF A SUBSTANCE

    The heat that must be supplied or removed to change the phase

    of a mass mof a substance is

    mLQ

    latent heat

    SI Units of Latent Heat: J/kg

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 41

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 42

    Example 14 Ice-cold Lemonade

    Ice at 0oC is placed in a Styrofoam cup containing 0.32 kg of lemonade

    at 27oC. The specific heat capacity of lemonade is virtually the same as

    that of water. After the ice and lemonade reach and equilibrium

    temperature, some ice still remains. Assume that mass of the cup is

    so small that it absorbs a negligible amount of heat.

    lemonadebylostHeat

    lemonade

    icebygainedHeat

    iceTcmmLf

    12.8 Heat and Phase Change: Latent Heat

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    PHYS222 LSSU Bazlur Slide 43

    lemonade

    bylostHeat

    lemonade

    icebygainedHeat

    iceTcmmLf

    kg11.0kgJ103.35C0C27kg32.0CkgJ4186

    L

    5

    f

    lemonadeice

    Tcmm

    12.9 Equilibrium Between Phases of Matter

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    PHYS222 LSSU Bazlur Slide 44

    The pressure of vapor that coexists in equilibrium with the liquid is

    called the equi l ibr ium vapor pressureof the liquid.

    12.9 Equilibrium Between Phases of Matter

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    PHYS222 LSSU Bazlur Slide 45

    Only when the temperature and vapor pressure correspond to a point

    on the curved line do the liquid and vapor phases coexist in equilibrium.

    12.9 Equilibrium Between Phases of Matter

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    PHYS222 LSSU Bazlur Slide 46

    Conceptual Example 16 How to Boil Water That is

    Cooling Down

    Shortly after the flask is removed from the burner,

    the boiling stops. A cork is then placed in the neck

    of the flask to seal it. To restart the boiling, should

    you pour hot or cold water over the neck of the

    flask?

    12.9 Equilibrium Between Phases of Matter

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    12.9 Equilibrium Between Phases of Matter

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    PHYS222 LSSU Bazlur Slide 48

    As is the case for liquid/vapor

    equilibrium, a solid can be in

    equilibrium with its liquid phase

    only at specific conditions oftemperature and pressure.

    12.10 Humidity

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    PHYS222 LSSU Bazlur Slide 49

    Air is a mixture of gases.

    The total pressure is the sum of the part ial pressuresof the component

    gases.

    The partial pressure of water vapor depends on weather conditions. It

    can be as low as zero or as high as the vapor pressure of water at the

    given temperature.

    100

    retemperatuexistingatwaterofpressurevapormEquilibriu

    orwater vapofpressurePartialhumidityrelativePercent

    To provide an indication of how much water vapor is in the air, weather

    forecasters usually give the relat ive hum idity :

    12.10 Humidity

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    Example 17 Relative Humidities

    One day, the partial pressure of water vapor is 2.0x103Pa. Using the

    vaporization curve, determine the relative humidity if the temperature

    is 32oC.

    12.10 Humidity

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    PHYS222 LSSU Bazlur Slide 51

    100

    retemperatuexistingatwaterofpressurevapormEquilibriu

    orwater vapofpressurePartialhumidityrelativePercent

    %42100Pa108.4

    Pa100.2humidityRelative

    3

    3

    12.10 Humidity

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    PHYS222 LSSU Bazlur Slide 52

    The temperature at which the relative humidity is 100% is called the dew

    point.

    12.10 Humidity

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    Force

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    PHYS222 LSSU Bazlur Slide 54

    A

    Force

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    PHYS222 LSSU Bazlur Slide 55

    A

    Force

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    A