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Lecture 11.1
Liquids and Intermolecular Forces The fundamental difference
between states of matter is the distance between particles. In
solids, particles are closely packed in an ordered array, their
positions are :ixed. In gases, particles are far apart and possess
complete freedom of motion. In liquids, particles are closely
packed but randomly oriented, and retain freedom of motion. Table
11.1 lists properties of solids, liquids and gases. Condensed phase
term given to solid and liquid states since particles are closer
together. The state a substance is in at a particular temperature
and pressure depends on two antagonistic entities: (a) the kinetic
energy of the particles, and (b) the strength of the attractions
between the particles.
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The :igure distinguishes intramolecular from intermolecular
attraction. The attractions between molecules (intermolecular
attractions) are not nearly as strong as the intramolecular
attractions that hold compounds together. However, this
intermolecular attractions are strong enough to control the
physical properties of substances. These properties include boiling
and melting points, vapor pressures and viscosities. Intermolecular
forces are referred to as van der Waals forces; there are three
types: (a) Dipoledipole interactions (b) Hydrogen bonding (c)
London dispersion forces
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London Dispersion Forces Simply called dispersion forces, are
attractions between an instantaneous dipole and an induced dipole.
Instantaneous dipole can develop temporarily when the electrons in
an atom or molecule are distributed unsymmetrically about the
nucleus because of the constant motion of the electrons.
The tendency of an electrons to be distorted or unsymmetrically
distributed is called polarizability. Induced dipole forces result
when an ion or a dipole induces a dipole in an atom or a molecule
with no dipole. These are weak forces. Dispersion forces are
present in all molecules, whether they are polar or nonpolar.
nucleus
electrons
+ - unsymmetrical distribution symmetrical distribution
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Factors Affecting the Strength of London Dispersion Forces
The shape of the molecule: long, skinny molecules (like
n-pentane) tend to have stronger dispersion forces than short, fat
ones (like neopentane). This is due to the increased surface area
in n-pentane. Molecular weight or molar mass of the molecule: The
strength of dispersion forces tends to increase with increased
molecular weight. Larger atoms have larger electron clouds that are
easier to polarize. Boiling point is a property that measures
strength of intermolecular forces; the graph below shows increasing
boiling point with increasing atomic weight indicating increasing
dispersion forces.
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DipoleDipole Interactions Molecules that have permanent dipoles
are attracted to each other. The positive end of one is attracted
to the negative end of the other, and vice versa. These forces are
only important when the molecules are close to each other. The more
polar the molecule, the higher its boiling point.
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Which have a greater effect, dipole dipole interactions or
dispersion forces? If two molecules are of comparable size and
shape, dipoledipole interactions will likely be the dominating
force. If one molecule is much larger than another, dispersion
forces will likely determine its physical properties. The nonpolar
series (SnH4 to CH4) follow the expected trend. The polar series
follow the trend until you get to the smallest molecules in each
group.
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Hydrogen Bonding The dipoledipole interactions experienced when
H is bonded to N, O, or F are unusually strong, these interactions
are called hydrogen bonding. Hydrogen bonding arises in part from
the high electronegativity of nitrogen, oxygen, and :luorine.
IonDipole Interactions Iondipole interactions are important in
solutions of ions. The strength of these forces is what makes it
possible for ionic substances to dissolve in polar solvents.
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Use the :low-chart to determine the intermolecular forces in a
molecule
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Physical Properties Affected by Intermolecular Forces
Intermolecular forces control how well molecules stick together.
This affects many of the measurable physical properties of
substances:
Melting and Boiling Points If molecules stick together more,
they'll be harder to break apart Stronger intermolecular forces
higher melting and boiling points Viscosity Viscosity is a measure
of how well substances :low; resistance of a liquid to :low; It is
related to the ease with which molecules can move past each other.
Stronger intermolecular forces higher viscosity. Viscosity
decreases with higher temperature.
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Surface Tension Surface tension is a measure of the toughness of
the surface of a liquid; results from the net inward force
experienced by the molecules on the surface of a liquid Stronger
intermolecular forces higher surface tension. Vapor Pressure This
is a small amount of gas that is found above all liquids. Stronger
intermolecular forces Lower vapor pressure. Sample Problem 1: In
which of these substances is hydrogen bonding likely to play an
important role in determining physical properties: methane (CH4),
hydrazine (H2NNH2), methyl :luoride (CH3F), hydrogen sul:ide (H2S)?
Why? Solution: The answer is hydrazine, H2NNH2S, since hydrogen
bonding usually occurs only when the hydrogen is covalently bonded
to N, O, or F. Sample Problem 2: List the substances BaCl2, H2, CO,
HF, and Ne in order of increasing boiling point. Solution: The
boiling point depends in part on the attractive forces in each
substance. We need to order these according to the relative
strengths of the different kinds of intermolecular attractions. The
attractive forces are stronger for ionic so BaCl2 should have the
highest boiling point.
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Sample Problem 2 continued: H2, CO and HF are covalent
molecules, CO and HF are polar covalent, the polarity in H-F is
stronger than CO, therefore HF has a higher boiling point than CO.
In Ne and H2 are non-polar molecules, Ne has a higher mass than H2.
The answer is: H2 < Ne < CO < HF < BaCl2 Energy Changes
Associated with Phase Change
Heat of fusion is the amount of energy required to change a
solid at its melting point to a liquid. Heat of vaporization is the
amount of energy required to change a liquid at its boiling point
to a gas. Heat of sublimation is the amount energy required to
change a solid directly to a gas. The heat added to the system at
the melting and boiling points goes into pulling the molecules
farther apart from each other. The temperature of the substance
does not rise during a phase change.
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Sample Problem 3: Calculate the enthalpy change upon converting
1.00 mol of ice at -25 C to steam at 125 C under a constant
pressure of 1 atm. The speci:ic heats of ice, liquid water, and
steam are 2.03 J/g-K, 4.18 J/g-K, and 1.84 J/g-K, respectively. For
H2O, Hfus = 6.01 kJ/mol and Hvap = 40.67 kJ/mol. Solution: Ice at
-25 C to ice at 0 C: Ice 0 C to water at 0 C: Water at 0 C to water
at 100 C: Water at 100 C to water vapor at 100 C : Water vapor at
100 C to water vapor at 125 C: Total H = 0.914 + 6.01 + 7.52 + 40.7
+ 0.828 = 56.0 kJ
! = 1.00!!"#!!! 18.0!!!"# !!2.03 !! ! ! 0 !25 !! = 914!!=
0.914!!" ! = 1.00!!"#!!! 6.01!!"!"# = 6.01!!"
! = 1.00!!"#!!! 18.0!!!"# !!4.18 !! ! ! 100 0 !! = 7520!! =
7.52!!" ! = 1.00!!"#!!! 40.67!!"!"# = 40.7!!" ! = 1.00!!"#!!!
18.0!!!"# !!1.84 !! ! ! 125 100 !! = 828!!= 0.828!!"
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Vapor Pressure At any temperature some molecules in a liquid
have enough energy to escape to the gaseous state. As the
temperature rises, the fraction of molecules that have enough
energy increases. As more molecules escape from the liquid to the
gaseous state, the pressure (called the vapor pressure) exerted by
these gases over the liquid increases. When the liquid molecules
evaporate at the same rate as the vapor molecules condensing the
liquid and vapor reach a state of dynamic equilibrium. The
temperature at which the vapor pressure equals atmospheric pressure
is called the boiling point of the liquid. The temperature at which
the vapor pressure is at 760 torr is called the normal
boiling point of the liquid.
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Phase Diagram Phase diagrams display the state of a substance at
various pressures and temperatures, and the places where equilibria
exist between phases. The liquidvapor interface starts at the
triple point (T), at which all three states are in equilibrium, and
ends at the critical point (C), above which the liquid and vapor
are indistinguishable from each other. Each point along this line
is the boiling point of the substance at that pressure. The
interface between liquid and solid marks the melting point of a
substance at each pressure. Below the triple point the substance
cannot exist in the liquid state. Along the solidgas line those two
phases are in equilibrium; the sublimation point at each pressure
is along this line.
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Phase Diagram of Water The slope of the solidliquid line is
negative. This means that as the pressure is increased at a
temperature just below the melting point, water goes from a solid
to a liquid
Phase Diagram of Carbon Dioxide Carbon dioxide cannot exist in
the liquid state at pressures below 5.11 atm; CO2 sublimes at
normal pressures.
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Sample Problem 4: Use the :igure in slide 14 to estimate the
boiling point of diethyl ether under an external pressure of 0.80
atm. Answer: Since 0.80 atm = 610 torr, the boiling point is at 27
oC Sample Problem 5: Use the phase diagram for methane, CH4, shown
in the :igure: (a)What are the approximate temperature and pressure
of the critical point? (b) What are the approximate temperature and
pressure of the triple point? (c) Is methane a solid, liquid, or
gas at 1 atm and 0 C? (d) If solid methane at 1 atm is heated while
the pressure is held constant, will it melt or sublime? (e) If
methane at 1 atm and 0 C is compressed until a phase change occurs,
in which state is the methane when the compression is complete?
Answers: (a) The critical point is at approximately -80 C and 50
atm. (b) The triple point is at approximately -180 C and 0.1 atm.
(c) Gas (d) Melt (e) Gas
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Liquid Crystals Some substances do not go directly from the
solid state to the liquid state. In the intermediate state called
liquid crystalline state, some traits of solids and some of liquids
are exhibited by the molecule. Liquid crystals have properties
between those of conventional liquid and those of solid crystal.
For instance, a liquid crystal may :low like a liquid, but its
molecules may be oriented in a crystal-like way. Liquid crystals
can exhibit color changes with changes in temperature. Examples of
liquid crystals can be found both in the natural world and in
technological applications. Most contemporary electronic displays
use liquid crystals.
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Unlike liquids, molecules in liquid crystals have some degree of
order. In nematic liquid crystals, molecules are only ordered in
one dimension, along the long axis. In smectic liquid crystals,
molecules are ordered in two dimensions, along the long axis and in
layers.
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In cholesteryl liquid crystals, nematic-like crystals are
layered at angles to each other.
End of Chapter 11