Gases
Gases
Gases
Characteristics of Gases
Unlike liquids and solids, gases
Characteristics of Gases
1. Gases can be compressed into smaller volumes; that
is, their densities can be increased by applying
increased pressure.
Characteristics of Gases
1. Gases diffuse into one another, and so samples of gas placed in
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Pressure
Pressure is defined as
the amount of force
per unit area.
F
P=
A
Atmospheric
pressure is the
weight of air per
unit of area.
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Units of Pressure
Pascals
1 Pa = 1 N/m2
Bar
1 bar = 105 Pa = 100 kPa
Units of Pressure
mm Hg or torr
These units are literally the
difference in the heights
measured in mm (h) of two
connected columns of
mercury.
Atmosphere
1.00 atm = 760 torr
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Manometer
This device is used to
measure the difference in
pressure between
atmospheric pressure and
that of a gas in a vessel.
Standard Pressure
Normal atmospheric pressure at sea level is referred to as
standard pressure.
It is equal to
1.00 atm
The four variables needed to define the state of a gas are P, V, T, & n
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The four variables needed to define the state of a gas are P, V, T, & n
As P and V are
inversely proportional
A plot of V versus P
results in a curve.
Since PV = k
V = k (1/P)
This means a plot of
V versus 1/P will be
a straight line.
=
Q1. A sample of gas occupies 12 L under a pressure of 1.2
atm. What would its volume be if the pressure were
increased to 2.4 atm?
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i.e.,
V =k
T
=
which is the more useful form of Charless Law. This relationship
is valid only when temperature,T, is expressed on an absolute
(usually the Kelvin) scale.
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V = kn
1 2
=
( , )
1 2
The standard molar volume of an ideal gas is taken to be 22.414
liters per mole at STP.
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Ideal-Gas Equation
So far weve seen that
V 1/P (Boyles law)
V T (Charless law)
V n (Avogadros law)
nT
V
P
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Ideal-Gas Equation
The relationship
then becomes
nT
V
P
nT
V=R
P
or
PV = nRT
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Ideal-Gas Equation
The constant of
proportionality is
known as R, the gas
constant.
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Densities of Gases
If we divide both sides of the ideal-gas
equation by V and by RT, we get
n
P
=
V
RT
Densities of Gases
We know that
moles molecular mass = mass
n=m
So multiplying both sides by the
molecular mass ( ) gives
m P
=
V RT
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Densities of Gases
Mass volume = density
So,
m P
d=
=
V RT
=
. 1
=
. 2
,
, =
. 3
,
. 3 int 2
=
=
(
( =
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Molecular Mass
We can manipulate the density equation to
enable us to find the molecular mass of a
gas:
P
d=
RT
Becomes
dRT
= P
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Daltons Law of
Partial Pressures
The total pressure of a mixture of gases
equals the sum of the pressures that each
would exert if it were present alone.
In other words,
Ptotal = P1 + P2 + P3 +
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Partial Pressures
Kinetic-Molecular Theory
This is a model that aids
in our understanding of
what happens to gas
particles as
environmental
conditions change.
2.
4.
The collisions between gas molecules and with the walls of the
container are perfectly elastic: the average kinetic energy of the
molecule does change with time or the the total energy is
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The KMT
So how does KMT explains the observable gas properties?
Pressure: This results from the collision of the molecules with the wall of the
container. The magnitude of pressure depends on how often (frequency) or how
forceful (speed) the molecules collide with the container.
The absolute temperature is a measure of the average kinetic energy of the
molecule. That is molecular motion increases with increasing temp
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The KMT
So how does KMT explains the observable gas properties?
We can relate pressure to speed by the equation:
1
=
2
3
= ; = tan; = ;
u = ()
Rearranging,
pV
1
nNA mc 2
3
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Please note that although the molecules in a sample of gas have average kinetic
energy and hence average speed, the individual molecules have varying speeds
Root mean square velocity is the speed of a molecule possessing average
kinetic energy
It is the measure of the speed of particles in a gas that is most convenient for
problem solving within the kinetic theory of gases because it is related directly to
the kinetic energy of the gas molecules
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The equation above relates the speed of a gas to its molar mass
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(the smell of rotten eggs) is released in a large room, the odor can
eventually be detected throughout the room. If a mixture of gases is
placed in a container with thin porous walls, the molecules effuse through
the walls. Because they move faster, lighter gas molecules effuse through
the tiny openings of porous materials faster than heavier molecules.
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Effusion
Effusion is the
escape of gas
molecules
through a tiny
hole into an
evacuated
space.
Effusion
The difference in the
rates of effusion for
helium and nitrogen,
for example, explains
a helium balloon
would deflate faster.
Diffusion
Diffusion is the spread
of one substance
throughout a space or
throughout a second
substance.
Grahams law defines the relationship of the speed of gas diffusion (mixing of
gases due to their kinetic energy) or effusion (movement of a gas through a tiny
opening) and the molecular mass (or density). In general, the lighter the gas, the
faster is its rate of effusion. Normally we use a comparison of the effusion rates of
two gases with the specific relationship being:
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In the real world, no gas is truly ideal. All gas particles have some
volume, however small it may be, because of the sizes of their atoms
and the lengths of their bonds. All gas particles also are subject to
intermolecular interactions.
Despite that, most gases will behave like ideal gases at many
temperature and pressure levels.
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Real Gases
In the real world, the
behavior of gases only
conforms to the idealgas equation at
relatively high
temperature and low
pressure.
Nonideal gas behaviour (deviation from the predictions of the ideal gas
laws) is most significant at high pressures and/or low temperatures,
that is, near the conditions under which the gas liquefies.
Real Gases
Even the same gas will
show wildly different
behavior under high
pressure at different
temperatures.
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As a consequence, the pressure that the gas exerts, Pmeasured, is less than the
pressure it would exert if attractions were truly negligible, Pideally exerted.
To correct for this, we subtract a correction factor, n2a/V2, from the ideal
pressure
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= +
We can then substitute both corrections into ideal gas law, PV =nRT
+
This is the van der Waals equation. In this equation, P, V, T, and n represent
the measured values of pressure, volume, temperature.
When a and b are both zero, the van der Waals equation reduces to the ideal
gas equation.
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Good morning, May I welcome you from the holiday with this:
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Two tanks are connected by a closed valve. Each tank is filled with gas as
shown, and both tanks are held at the same temperature. We open the
valve and allow the gases to mix.
(a) After the gases mix, what is the partial pressure of each gas, and what
is the total pressure?
(b) What is the mole fraction of each gas in the mixture?
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A gas
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