Chapter 5
Temperature (T)
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The measure of hotness or coldness. |
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The temperature of matter depends on
the average kinetic energy of atoms and molecules. |
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Feelings of hot and cold depend on
temperature and conductivity. |
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Touch metal and wood, which feels
warmer? |
Kinetic Energy and
Temperature
The Sun
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For example on the sun, the temperature
is very high, in fact so high that atoms and molecules do not even
exist! The sun is a Plasma. |
Temperature scales.
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We normally measure temperature with
three different temperature scales, or units. |
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Fahrenheit, oF, (British) |
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Celsius, oC, (Original
Metric) and |
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Kelvin, K (no degrees) (Modern Metric) |
Celsius and Fahrenheit
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In the Celsius Scale water boils at 100
deg. And freezes at 0 deg. |
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In Fahrenheit water boils at 212, and
freezes at 32, |
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so 100 oC = 212 –32 or 180 oF. |
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The ratio of the sizes is 100/180 = 5/9 |
Converting from oF
to oC
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To convert from oF use |
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oC = 5/9 x (oF-32) |
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E.G. convert 50 oF to oC. |
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50 deg.F = 5/9 (50-32) = 5/9 x 18 = |
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5 x 18/9 = 10 deg.C |
Converting from C to F
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To convert from C use F= 9/5C + 32 |
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For example 80 C = 9/5 x 80 + 32 |
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= (9 x 80/5) +32 = (9 x 16) + 32 |
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= 144 + 32 = 176 |
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80 oC = 176 oF |
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Absolute Zero
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After the Celsius scale was devised in
the 1800’s, it was discovered through the study of gases, that there seemed
to be a limit on how low temperature could go. |
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This was called absolute zero. |
Kelvin Degrees
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Same size units as o C |
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Starts with zero at absolute zero
instead of the freezing of water. |
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First called the absolute temperature |
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Later renamed The Kelvin Scale, in
honor of Lord Kelvin. (Not oK, just K or Kelvins!) |
Converting from deg C to
K
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K = C + 273 |
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Kelvin temperature is proportional to
the average kinetic energy of the constituent particles. |
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30 deg C = ? K K = 30 + 273 = 303 |
Converting from deg K to C
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C = K - 273 |
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430
K = ?C C = 430 - 273 = 157 o
C |
Hot Air
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On Earth higher air temperatures mean
the air molecules are moving faster,) i.e. they have more kinetic energy (KE
= ˝ mv2 ) |
Air KE vs. Temperature
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At 0 K, there would be no air motion |
Planetary Atmosphere
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A planet’s gravity and temperature
govern the composition of its atmosphere. |
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Higher temperature means higher energy
of particles in the atmosphere, meaning more kinetic energy and greater
potential to escape gravity. |
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Greater gravity means they have less
chance to escape the planet. |
Thermal Expansion
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Most objects expand when they are
heated. |
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Solids expand in amounts dependant on
their length, L and the change in temperature, DT, but the change in length also depends on the composition
of the material. |
Equation for Thermal
Expansion
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The equation is Dl=al DT |
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l=length of the material, Dl = change in
length, and DT = change in temperature of the object. |
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a, the coefficient of linear expansion, we have to measure or look up
for a given material. |
Different Objects Expand
Different Amounts
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a, The coefficient of linear expansion varies greatly. Some things expand a lot, others a little.
(See table 5.2 p. 179) |
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E.G. a for
Al 25, Brick 9, Ice 51, Glass 9 |
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(all x 10-6/deg.C) |
Windows.
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If we put glass in a metal frame in a
window subject to large temperature variations we will have a problem. |
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Aluminum expands and contracts faster
and more than the glass. |
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If the window cools suddenly the
aluminum will contract and shrink and may break the glass. |
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Thermal Expansion
Problem.
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Dl=al DT :Change in length = coef. of exp. x length x change in temp. |
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Example: a for Al = 25 x 10-6/oC, Tf=100 oC
T0=50 oC |
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For lo = 2 m, DT = 50 oC Note Negative DT means contraction! |
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Dl = 2m x 25 x 10 -6 /oC x 50 oC=2500x
10-6 |
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= 2.5 x 10 -3 = .0025 m =
2.5 mm (lf =2.0025m) |
Bimetallic Strip
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2 metals bonded together with different
coefficients of linear expansion. |
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When heated it bends because of the
different expansions. |
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Used in thermostats and
thermometers see p.181 |
Noteworthy properties of
water
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its high specific heat capacity |
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unusual thermal expansion properties). |
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Water contracts on cooling, but between
1 and 0, it expands.(p 182) |
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Thus just before freezing it rises,
making ice on the top of the lake, etc. |
Use the ideal gas law.
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PV =kT |
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Pressure x Volume is proportional to
Kelvin Temperature in a gas |
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We can also state this as |
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PV/T = constant |
Heat (Q)
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The form of energy that is transferred
between two substances at different temperatures. |
Heat and Internal energy
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Units of heat and early confusion. |
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Calorie: Heat necessary to raise one G
of water 1 deg. C. |
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KG Cal or big Calorie. |
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Caloric… Heat was something in itself,
separate from matter and energy. |
Internal energy (U)
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The sum of the kinetic energies and
potential energies of all the atoms and molecules in a substance. |
First law of
thermodynamics
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The change in internal energy of a
substance equals the work done on it plus the heat transferred to it. |
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DU=work + Q |
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Change in internal energy = work + heat
change ( + or -) |
First Law Problem
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For example 50 Joules of heat are added
to a substance and 30 Joules of work are done on it. What is the change in energy? |
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DU=work + Q |
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DU = 30 + 50 = 80 Joules. |
Three types of heat
transfer
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Conduction The transfer of heat by
direct contact between atoms and molecules |
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Convection The transfer of heat by
buoyant mixing in a fluid. |
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Radiation Heat transfer in the form of
electromagnetic energy. |
Conduction
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The metal worker wears insulated gloves
to slow down conduction to his hands from the hot tongs he is holding. |
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The heat is conducted from the hot
metal through the cup through the tongs, and then through the gloves. |
Convection
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Wind passes by your hot body, picks up
the heat and takes it away with the air. |
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Convection occurs in solids or liquids. |
Radiation
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See the heat radiating out from the hot
metal. |
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Radiation can travel through a vacuum. |
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Light is radiation. |
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Some radiation we can not see, for
example heat radiation or infra-red radiation. |
Specific Heat Capacity
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Adding heat to a substance generally
raises its temperature, as long as it does not change phase. |
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We find if we double the heat added we
double the temperature rise for a certain amount and type of substance. |
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This can be expressed mathematically
like this: Q= CmDT |
Diagram of Heat Capacity
Calculations of heat
transfer using specific heat capacity.
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Q= CmDT :Heat Gained
= Heat Cap. x mass x change in Temp. |
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For ice, C = 2000 J/Kg oC |
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To raise 10Kg by 20 oC we need |
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Q = 2000 x 10 x 20 (J/(Kg oC)
x kg x oC) |
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Q = 400,000 Joules! |
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Phase transitions
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Changing from liguid, solid, or gaseous
form to one of the other forms. E.G.
liguid to gas |
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The temperature stays constant during a
phase transition. |
Latent Heat of Fusion
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Heat necessary to melt 1 kg of a
substance |
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Sample Problem
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The latent heat of fusion of ice is 334,000 joules. |
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How much heat is released when 4 kilos
of ice melts? |
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Q = m x Hf = 4 kg x 334,000 J/kg = |
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1.336 x 106 J |
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Latent Heat of
Vaporization.
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Heat necessary to turn 1kg of a
substance from liguid to vapor. |
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Heat of vaporization of water is
2,260,000 J/kg |
Humidity
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The mass of water vapor in the air
per unit volume. The density of water vapor in the air. |
Saturation Density.
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The amount of water absorbed by air
depends on the temperature and pressure. |
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Higher temperature air can hold more
water. |
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The saturation density is the amount of
moisture that water can hold at that temperature. |
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Relative humidity
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Humidity expressed as a percentage of
the saturation density. |
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See page 202 for chart and 203 for
graph of saturation densities, then divide your humidity by this number |
Rel. Hum Problem
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The humidity at 10 deg. C is .006 kg/cu
m |
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what is the relative humidity? |
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From the chart p 202 sat. density = .01
at 10 Deg.C |
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Rel. Hum= .006/.01 = .60 = 60% |
Dew point
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The temperature at which water in the
air condenses. |
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From the previous example for a
humidity of .6 kg/cu.m and T = 10 deg.C |
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On the graph p. 203 we find the dew
point for .6kg/cu.m to be 5 deg.C |
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Therefore, when this air cools to 5
deg. C there will be dew, fog, rain, snow, etc. |
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Second law of thermodynamics
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No device can be built that will
repeatedly extract heat from a heat source and deliver mechanical work or
energy without ejecting some heat to a lower-temperature reservoir. |
Explain how refrigerators
and heat pumps work.
Heat engine
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A device that converts heat into
mechanical energy or work. It absorbs heat from a hot source such as burning
fuel, converts some of this energy into usable mechanical energy or work, and
outputs the remaining energy as heat at some lower temperature. |
Normal Efficiency
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Eff = Output/Input |
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Efficiency = Work or Energy
Output/Input |
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Efficiency Problem.
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An elevator uses 500 Joules to do 350
Joules of useful work. What is it’s
efficiency? |
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E = Wout/Win = 350/ 500J = .7 or 70% |
Carnot Efficiency
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Ti-To /Ti =Carnot Eff. (Input Temp – Output
Temp/ Input Temp.) |
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as a % = 100 x(Tin - T out)/ Tin |
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Theoretical limit to the efficiency of
a heat system. See problem #27. |
Entropy.
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The disorder or entropy of the universe
is increasing. |
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