Chapter 10 Thermal Physics. Heat The exchange of energy between objects because of temperature...
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Transcript of Chapter 10 Thermal Physics. Heat The exchange of energy between objects because of temperature...
![Page 1: Chapter 10 Thermal Physics. Heat The exchange of energy between objects because of temperature differences is called heat Objects are in thermal contact.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bff31a28abf838cbc761/html5/thumbnails/1.jpg)
Chapter 10
Thermal Physics
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Heat The exchange of energy between
objects because of temperature differences is called heat
Objects are in thermal contact if energy can be exchanged between them
Thermal equilibrium exists when two objects in thermal contact with each other cease to exchange energy
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Zeroth Law of Thermodynamics
If objects A and B are separately in thermal equilibrium with a third object, C, then A and B are in thermal equilibrium with each other.
Allows a definition of temperature
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Temperature from the Zeroth Law Two objects in thermal equilibrium
with each other are at the same temperature
Temperature is the property that determines whether or not an object is in thermal equilibrium with other objects
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Pressure-Temperature Graph
All gases extrapolate to the same temperature at zero pressure
This temperature is absolute zero
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Modern Definition of Kelvin Scale Defined in terms of two points
Agreed upon by International Committee on Weights and Measures in 1954
First point is absolute zero Second point is the triple point of water
Triple point is the single point where water can exist as solid, liquid, and gas
Single temperature and pressure Occurs at 0.01º C and P = 4.58 mm Hg
The temperature of the triple point on the Kelvin scale is 273.16 K
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Some KelvinTemperatures
Note, this scale is logarithmic
Absolute zero has never been reached
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Comparing Temperature Scales
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Converting Among Temperature Scales
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Thermal Expansion The thermal expansion of an object is a
consequence of the change in the average separation between its constituent atoms or molecules
At ordinary temperatures, molecules vibrate with a small amplitude
As temperature increases, the amplitude increases This causes the overall object as a whole to
expand
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Linear Expansion For small changes in temperature
, the coefficient of linear expansion, depends on the material See table 10.1 These are average coefficients; they
can vary somewhat with temperature
α
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Applications of Thermal Expansion – Bimetallic Strip
Thermostats Use a bimetallic strip Two metals expand differently
Since they have different coefficients of expansion
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Area Expansion Two dimensions
expand according to
is the coefficient of area expansion
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Volume Expansion Three dimensions expand
For liquids, the coefficient of volume expansion is given in the table
α=βΔβ=Δ
3,solidsfor
tVV o
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Example
Determine the increase in ocean depth due to linear expansion from an increase of 1 oC owing to global warming effects. Assume a current average ocean depth of Lo = 4000 m, and use α = 6.90 x 10-5 (oC)-1.
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Unusual Behavior of Water
As the temperature of water increases from 0 ºC to 4 ºC, it contracts and its density increases
Above 4 ºC, water exhibits the expected expansion with increasing temperature
Maximum density of water is 1000 kg/m3 at 4 ºC
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Ideal Gas A gas does not have a fixed volume or
pressure In a container, the gas expands to fill the
container Most gases at room temperature and
pressure behave approximately as an ideal gas Collection of atoms or molecules that move
randomly Exert no long-range force on one another Each particle is individually point-like
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Moles It’s convenient to express the amount of
gas in a given volume in terms of the number of moles, n
One mole is the amount of the substance that contains as many particles as there are atoms in 12 g of carbon-12
massmolar
massn =
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Avogadro’s Number The number of particles in a mole
is called Avogadro’s Number NA=6.02 x 1023 particles / mole Defined so that 12 g of carbon
contains NA atoms
The mass of an individual atom can be calculated:
Aatom N
massmolarm =
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Avogadro’s Number and Masses The mass in grams of one Avogadro's
number of an element is numerically the same as the mass of one atom of the element, expressed in atomic mass units, u
Carbon has a mass of 12 u 12 g of carbon consists of NA atoms of
carbon Holds for molecules also
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Ideal Gas Law PV = n R T
R is the Universal Gas Constant R = 8.31 J / mole.K R = 0.0821 L. atm / mole.K Is the equation of state for an ideal
gas T is in Kelvin!
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Ideal Gas Law, Alternative Version P V = N kB T
kB is Boltzmann’s Constant kB = R / NA = 1.38 x 10-23 J/ K N is the total number of molecules
n = N / NA
n is the number of moles N is the number of molecules
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Example
An ideal gas at 20 oC and pressure 1.5 x 105 Pa is in a container of volume 1.0 L.
1. Determine the number of moles of gas. (R=8.31 J/mol/K)
2. If the gas pushes against a piston, expanding to twice its volume with a drop to atmospheric pressure (1.01 x 105 Pa), what is the final temperature?
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Kinetic Theory of Gases – Assumptions
The number of molecules in the gas is large and the average separation between them is large compared to their dimensions
The molecules obey Newton’s laws of motion, but as a whole they move randomly
The molecules interact only by short-range forces during elastic collisions
The molecules make elastic collisions with the walls The gas under consideration is a pure substance, all
the molecules are identical
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Pressure of an Ideal Gas The pressure is
proportional to the number of molecules per unit volume and to the average translational kinetic energy of a molecule
€
P =2
3
N
V
⎛
⎝ ⎜
⎞
⎠ ⎟1
2mv 2
⎛
⎝ ⎜
⎞
⎠ ⎟
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Molecular Interpretation of Temperature Temperature is proportional to the
average kinetic energy of the molecules
The total kinetic energy is proportional to the absolute temperature
Tk2
3mv2
1B
2 =
nRT2
3KEtotal =
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Internal Energy In a monatomic gas, the KE is the only
type of energy the molecules can have
U is the internal energy of the gas In a polyatomic gas, additional
possibilities for contributions to the internal energy are rotational and vibrational energy in the molecules
nRT2
3U=
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Speed of the Molecules Expressed as the root-mean-square
(rms) speed
At a given temperature, lighter molecules move faster, on average, than heavier ones Lighter molecules can more easily reach
escape speed from the earth
M
TR3
m
Tk3v Brms ==
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Quick Quiz One container is filled with argon gas
and another with helium gas. Both are at the same temperature. Which atoms have the higher rms speed?
1. Argon2. Helium3. Same speed4. Cannot tell
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Some rms Speeds
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Maxwell Distribution A system of gas
at a given temperature will exhibit a variety of speeds
Three speeds are of interest: Most probable Average rms