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Chapter 11: Properties of Gases

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Title: Chapter 11: Properties of Gases


1
Chapter 11 Properties of Gases
  • Gases have a number of properties that are very
    different from liquids and solids
  • Gases are compressible
  • Gases exert a pressure
  • Gas pressure depends on the amount of confined
    gas
  • Gases fill their container
  • Gases mix freely with each other
  • Gas pressure increases with temperature

2
The qualitative observations of the properties of
gases leads to the conclusion that a gas is
comprised of widely spaced molecules in rapid
motion. Collisions of molecules with the walls
are responsible for the gas pressure.
  • This simple model of gases is the basis of the
    kinetic-molecular theory (discussed in Section
    7.2)

3
  • Recall the pressure is a force per unit area
  • The earth exerts a gravitational force on
    everything with mass near it
  • What we call weight is the gravitational force
    acting on an object
  • The pressure due to air molecules colliding with
    an object is called the atmospheric pressure

4
Atmospheric pressure is measured with a
barometer. A Torricelli barometer consists of a
glass tube sealed at one end, about 80 cm in
length. The tube is filled with mercury, capped,
inverted, and the capped end immersed in a pool
of mercury. When the cap is removed the
atmosphere supports a the column of mercury about
760 mm high.
5
  • The height of the mercury column varies with
    altitude
  • The average pressure at sea level or the standard
    atmosphere (atm) was defined as the pressure
    needed to support a column of mercury 760 mm high
    measures at 0oC
  • The SI unit of pressure is the pascal (Pa)

6
  • You may encounter a number of pressure units
  • The standard atmosphere is
  • Chemical reactions often involve gases

7
  • A manometer is used to measure the pressure
    inside closed containers

Open-end manometer. (a) The pressure of the
trapped gas, Pgas equals the atmospheric
pressure, Patm. Trapped gas pressure (b) higher
and (c) lower than atmospheric pressure.
8

A closed-end manometer for measuring gas
pressures less than 1 atm. When constructed (a)
the tube is fully evacuated and mercury is
allowed to enter and fill the closed arm
completely. (a) Mercury flows out of the closed
arm when the bulb contains gas at low pressure.
The difference in mercury levels, PHg, is the
pressure of the confined gas, Pgas.
9
  • Mercury is so dense (13.6 g mL-1) that small
    pressure changes are difficult to measure
  • Other liquids can be used to make manometers

Columns of mercury and water that exert the same
pressure. Mercury is 13.6 times more dense than
water. Both columns have the same weight and
diameter, so they exert the same pressure.
10
  • Thus for a given difference in pressure, the
    difference in heights between the two levels is
    inversely proportional to the density of the
    liquid used in the manometer
  • There are four variables that affect the
    properties of a gas pressure, volume,
    temperature, and the amount of the gas
  • Simple experiments can be conducted that relate
    how these variables change
  • The gas laws summarize these experiments

11

Compressing a gas increases its pressure. A
molecular view of what happens when a gas is
squeezed into a smaller volume. The number of
collisions with a given area of the walls
increases which causes the pressure to rise.
12

Robert Boyle studied how the volume of a fixed
amount of gas varies with pressure at constant
temperature. (a) Air trapped in a J-tube by
mercury. (b) As more mercury is added, the
pressure of the trapped gas increases and the
volume decreases.
13

(a) A typical graph of volume versus pressure
showing volume decreasing as pressure increases.
(b) A straight line is obtained when volume is
plotted against (1/P), which shows that
14
  • The relationship between volume and pressure is
    called Boyles law or the pressure-volume law
  • The volume of a given amount of gas held at
    constant temperature varies inversely with the
    applied pressure
  • The proportionality can be removed by introducing
    a proportionally constant, C

15
  • Boyles law is remarkably successful, especially
    for common laboratory conditions
  • However, no real gas obeys Boyles law exactly
    over a wide range of temperatures and pressures
  • The hypothetical gas that does exactly obey
    Boyles law is called an ideal gas
  • Real gases act more like ideal gases as their
    pressures decrease and temperatures increase

16
  • Jacques Alexander Charles studied how the volume
    of a gas sample varied with temperature

Charles law plots. Each line shows how the gas
volume changes with temperature for different
sized samples of the same gas.
17
  • When extrapolated to zero volume all the samples
    have the same temperature
  • This temperature is called absolute zero and is
    the basis of the Kelvin temperature scale
  • Charles law or the temperature-volume law can be
    expressed mathematically

18
  • Joseph Louis Gay-Lussac studied how the pressure
    and temperature of a fixed amount of gas at
    constant volume are related
  • Gay-Lussacs law or the pressure-temperature law
    states
  • The pressure of a fixed amount of gas held at
    constant volume is directly proportional to the
    Kelvin temperature
  • Mathematically this is

19
  • The three gas laws are often used in a single
    equation called the combined gas law
  • When using this equation the temperature must
    always be in kelvins
  • Alternate forms of the previous gas laws result
    when certain variables cancel

20
  • Problems involving the gas laws are important

21
  • Example What will be the the final pressure of a
    sample of oxygen with a volume of 850 m3 at 655
    torr and 25.0oC if it is heated to 80.0oC and
    given a final volume of 1066 m3?
  • ANALYSIS Use the combined gas law with
    temperature in kelvins.
  • SOLUTION

22
  • The law of combining volume states
  • When gases react at the same temperature and
    pressure, their combining volumes are in ratios
    of simple, whole numbers
  • Example
  • Amedeo Avogadro studied this and devised
    Avogadros principle
  • When measured at the same temperature and
    pressure, equals volumes of gases contain equal
    number of moles

23
  • A corollary to Avogadros principle is
  • The volume of a gas is directly proportional to
    its number of moles, n
  • Thus, the volume of one mole of any gas at
    standard temperature and pressure (STP) or 0oC
    and 1 atm is 22.4 L (a constant for all ideal
    gases)
  • This is called the standard molar volume of a gas

24
  • The combined gas law can be generalized to
    include changes in the number of moles of sample
  • The ideal gas law is

25
  • The molecular mass is obtained by taking the
    ratio of mass to moles, which could be determined
    using the ideal gas law
  • Gas densities (d), a ratio of gas mass to volume,
    can be calculated by taking the ratio of the
    molar mass to molar volume
  • Example The molar mass of oxygen is 32.0 g/mol.
    What is the density of oxygen at STP?

26
One mole of each gas occupies 22.4 at STP. Carbon
dioxide is more dense that oxygen due to molar
mass differences.
  • We now need to consider mixtures of gases
  • One useful way to describe a composition of a
    mixture is in terms of its mole fractions
  • The mole fraction is the ratio of the number of
    moles of a given component to the total moles of
    all components

27
  • For a mixture of A, B, substances, the mole
    fraction of substance i (Xi) is
  • This provides a convenient way to partition the
    total pressure of a mixture of gases
  • Daltons law of partial pressures states the
    total pressure of a mixture of gases is the sum
    of their individual partial pressures

28
  • For a system of only gases, mole fractions and
    partial pressure partition the total pressure in
    the same fashion
  • Gases are often collected over water in the
    laboratory
  • These (collected) gases are saturated with water

29
  • The space above any liquid contains some of the
    liquids vapor
  • The pressure this vapor exerts is called the
    vapor pressure

As the gas bubbles through the water, water vapor
gets into the gas so the total pressure inside
the bottle includes the partial pressure of the
water vapor.
30
  • The total pressure is the pressure of the gas
    plus the vapor pressure of water

Vapor pressure of water at various temperatures.
31
  • Example A sample of oxygen is collected over
    water at 20oC and a pressure of 738 torr. What is
    the partial pressure of oxygen?
  • ANALYSIS The partial pressure of oxygen is less
    than the total pressure. Get the vapor pressure
    of water from table 11.2 (page 478).
  • SOLUTION
  • Partial pressures can be used to calculate mole
    fractions

32
  • This is possible because the number of moles of
    each gas is directly proportional to its partial
    pressure
  • Using the ideal gas equation for each gas
  • For a given mixture of gases, the volume and
    temperature is the same for all gases
  • Using CV/RT gives

33
  • The partial pressure of a gas can be calculated
    using the total pressure and mole fraction

34
  • Gas volumes can be used in stoichiometry problems

35
  • Diffusion is the spontaneous intermingling of the
    molecules of one gas with another
  • Effusion is the movement of gas molecules through
    a tiny hole into a vacuum
  • The rates of both diffusion and effusion depend
    on the speed of the gas molecules
  • The faster the molecules, the faster diffusion
    and effusion occur
  • Thomas Graham studied effusion

36
  • He found that the effusion rate of a gas was
    inversely proportional to the square root of the
    density (d)
  • This is known as Grahams law
  • Where Mi is the molar mass of species i

37
  • The behavior of ideals gases can be explained
  • Diffusion (b) Effusion

38
  • Postulates of the Kinetic Theory of Gases
  • A gas consists of a large number of tiny
    particles that are in constant, random motion.
  • The gas particles themselves occupy a net volume
    so small in relation to the volume of their
    container that their contribution to the total
    volume can be ignored.
  • The collisions between particle and with the
    walls of the container are perfectly elastic.

39
  • Calculations show that PV is proportional to the
    average kinetic energy and the Kelvin
    temperature, thus
  • The kinetic theory also explains the gas laws

40

The kinetic theory and the pressure volume law
(Boyles law). When the gas volume is made
smaller going from (a) to (b), the frequency of
collisions per unit area of the containers wall
increases. Thus the pressure increases.
41

The kinetic theory and the pressure-temperature
law (Gay-Lussacs law). The pressure increases
from (a) to (b) as measured by the amount of
mercury that must be added to maintain a constant
volume.
42

The kinetic theory and the temperature-volume law
(Charles law). The pressure is the same in both
(a) and (b). At higher temperatures the volume
increases because the gas molecules have higher
velocities.
43
  • Grahams law requires that the rate of effusion
    for the different gases be compared at the same
    temperature and pressure
  • When different gases have the same temperature,
    they have the same average kinetic energy
  • The average kinetic energy can be expressed in
    terms of the average of the velocities squared or
    root mean square
  • For the two gases labeled 1 and 2

44
  • Note that heavier gases move slower than lighter
    gases

45
  • The rate of effusion is proportional to the
    average molecular speed, thus
  • The kinetic theory predicts that absolute zero is
    the temperature at which the average kinetic
    energy of an ideal gas is zero
  • Real gases exhibit non-ideal behavior

46
Deviation from the ideal gas law. A plot of PV/T
versus P for an ideal gas is a straight line. The
same plot for oxygen is not a straight line
  • Deviations from ideal behavior occur because
  • Gas molecules interact, and
  • Gas molecules occupy a finite volume.

47
  • J. D. van der Waals corrected the ideal gas
    equation in a simple, but useful, way

(a) In an ideal gas, molecules would travel in
straight lines. (b) In a real gas, the paths
would curve due to the attractions between
molecules.
48
  • He did this by modifying the measured pressure
    and volume of a real gas so it fits the ideal gas
    equation
  • The constants a and b are called the van der
    Waals constants

49
  • Table 11.3 (page 493) has a more complete set of
    van der Waals constants
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