Phases and Equilibrium
The States of Matter,
Molecular Stickiness, and Thermodynamics
The phases of matter represent 'classes' of the type of
molecular motion found at different temperatures. When the temperature is low, the motion of molecules is dominated by the fact that they stick together, and the result is a phase of matter that is rigid and dense. When the termperature is high, the motion of the molecules is dominated by their translational energy, so intermolecular forces can almost be ignored. At intermediate temperatures, molecules translate but still stick together.
Solids
(tightly-bound molecules)
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At low temperatures the nuclei of the atoms of a solid vibrate
about an equilibrium position but are trapped in their lattice positions, unable to flow or diffuse.
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The intermolecular forces are stronger than the average thermal
energy of the system.
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Long range radial and angular order (structure) are usually
present in single crystal solids. Even amorphous solids have relatively
good spatial ordering, especially over small distances, (10-100 molecules)
Liquids
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As the binding energy to the lattice site is overcome by
thermal energy, the molecules in the solid may slip past each other but
maintain close contact.
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The overall substance is fluid, but not very compressible.
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Some long range radial ordering persists, but usually only
over the size of a few molecular diameters
Gases (free motion)
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Gases are described by the Kinetic Theory of Gases. In this limit, gas molecules have negligible size, have no appeciable intermolecular forces, and are in continous, random motion.
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Gases have mean free paths that are larger than molecular
diameters, i.e. they are usually isolated but occasionally have collisions
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The state of a gas is universally, if approximately, described
by the Ideal Gas Equation of State.
Surfaces and Interfaces
At the edge of any solid or liquid (condensed phase) is a surface.
When two different types of matter are in contact, they share a surface called and interface.
An interface is where two phases of matter meet.
At a surface, molecules have neighbors of the same type only on one side.
Thus surface molecules are different from those in the bulk.
Bulk molecules have neighbors in all directions.
At an interface between a condensed phase and a gas or a vacuum, the molecules at the surface are unstable with respect to the bulk.
Why? Because attractive intermolecular forces must be broken to bring a molecule from the bulk to the surface and there is nothing there to give that energy back.
The number of molecules at the surface is proportional to the
surface area.
Surface Tension:
It takes energy to create a new surface of a solid or
liquid because one must move a molecule from the bulk to a site at the
surface and this takes energy. The amount of energy it takes to create
one unit of area (1 m2) of new surface is called the surface
tension, g, with units J/m2. Here
are some experimental surface tension data:
The Surface Tension of Various Interfaces
|
Interface (Temperature)
|
Surface Tension [mJ/m2]
|
|
Water / Air (20 oC)
|
72.75
|
|
Hg / Air (20 oC)
|
472
|
|
Benzene / Air (20 oC)
|
28.88
|
|
Water / Air (100 oC)
|
58.0
|
Viscosity:
Intermolecular forces manifest themselves not only in the surface tension tension of a liquid, but in the way a liquid flows.
The resistance to flow of a liquid is called the
liquid's viscosity .
The greater the viscosity, the "more slowly it flows".
The viscosity
of the oil lubricating your car engine is an important part of engine performance
and longevity. You change your oil when the viscosity of the engine oil 'breaks
down' or decreases. You use in different oil in your car during the winter than
in the summer because viscosity is effected by temperature.
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Viscosity is a measure of the ease with which molecules move
past one another.
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Viscosity depends on the attractive force between the molecules.
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Viscosity of a liquid decreases with increasing temperature
- the increasing kinetic energy overcomes the attractive forces and molecules
can more easily move past each other.
Some definitions
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Surface
is the edge or boundary of a material.
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Interface
is the region of contact between two phases.
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Surface tension
is the energy required to increase the surface area of a liquid (or
solid) by a unit amount, i.e J/m2
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Viscosity
is the resistance to the flow of a liquid. Solids don't have viscosity.
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Cohesive
forces bind molecules of the same type
together
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Adhesive
forces bind unlike molecules
Surface tension
determines the pressure inside of a bubble.
A free standing liquid bubble has gas on the inside and outside; Surface tension
will tend to make the bubble collapse on the gas inside
and thus cause an increase in pressure
inside. This increase in pressure can be derived (can you derive this
formula?):

This formula results from the observation that a
bubble
has two interfaces, the pressure
increase inside a drop
or cavitation, with only one interface, is only
2 g / r.
Cohesive and Adhesive forces and Curved
Surfaces also give rise to the phenomenon of Capillary
Action. We will assume a "contact angle" of 0 degrees to gert a simplified expression for capilary rise.
The more correct formula can be found here.

Phase Transitions
Our understanding of surface tension was made more complete by our
understanding of intermolecular forces, i.e., the energetics of making and
breaking of intermolecular bonds between molecular
'neighbors'.
Such energies can be determined experimentally by calorimetry,
or the measure of the heat flow during a chemical or physical process.
The heating of a sample of water from -25 to 125 oC
involves both the heat capacities of the pure phases but also the enthalpies
of the melting(fusion) and boiling(vaporization) of the water.
The enthalpy of the melting reaction and the boiling reaction
are both positive (endothermic). {Melting is sometimes called fusion}

Phase Transitions take energy because of the breaking (or making) of intermolecular 'bonds'.
Phase Transitions at a given temperature can reach
equilibrium, i.e. steady state. If you put any liquid in a sealed vessel and wait long enough,
the liquid will come into equilibrium with its vapor, and a constant (steady; dependent
only of the temperature) equilibrium vapor pressure will be established.
The equilibrium vapor pressure has an exponential temperature
dependence for any given substance. We can see this from the liquid/vapor equilibrium
curve:
Why does the vapor pressure increase with temperature so dramatically?
Because the fraction of the molecules in the sample with sufficient energy
to escape the shackles of their intermolecular forces depends
on the energy distribution that we have already seen in our study of gases.
The liquid / vapor equilibrium curve follows a simple
relation, because the amount of heat needed to vaporize the gas (molecular
stickiness) determines the vapor pressure. The equation governing the pressure
of a gas in equilibrium with a solid or a liquid can be derived from the
postulates of Thermodynamics and is a milestone in the fundamental understanding
of Phase Equilibria.
This relationship is called the Clausius-Clapeyron Equation (applicable
to both liquid/gas or solid/gas equilibrium curves) and has the form:
The Phase Diagram
Every substance can exist as a Solid, Liquid, or Gas, and so
Solid / Gas and Solid / Liquid and Liquid / Gas equilibria occur for
all substances at some temperature and pressure.
The phase diagram is a plot of all the equilibrium curves
between any two phases on a pressure temperature diagram:

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The shape of the Phase Diagram is Different in details depending
on the substances.
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There is only one place where all three phases of a pure
substance are at equilibrium. This is called the triple point [POINT A
on the diagram]. (The aliens, when we meet them, will know the pressure
and temperature of the triple point of water, do you?)
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The liquid / vapor equilibrium curve ends at a temperature
and pressure where gases and liquids are indistinguishable fluids. This
is called the critical point [POINT B on the diagram] and therefore has
a critical temperature and a critical pressure.
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At POINT C and POINT D on the diagram, two phases are in
equilibrium and off the line entirely there is only one stable phase of
the substance.
Comparison of Phase diagrams of Familiar Substances; Water(a)
and Dry Ice(b)

Liquids can be fleeting...
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Liquid water exists with its vapor at 1 atm pressure, but
liquid CO2 only exists above the pressure of 5.11 atm.
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In the lab (1 atm) we see that solid CO2 directly
dissociates into gaseous CO2 without making a liquid at all.
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Liquid CO2 is found in most CO2 fire
extinguishers, but only at a temperature below 31.1 oC, (88
F), where the liquid becomes inditinguishible from the gas.
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Liquid water persists to much higher temperatures, over 300
oC, but only at great pressure (100's of atm).
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Only water has a liquid / solid equibrium curve that has
a negative slope, i.e. it melts when you squeeze it. Water is unique in
its highly structured liquid phase (which is why life grows in water)
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