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Liquids and Solids Advanced Chemistry Chapter 10
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Page 1: Adv chem chapt 10

Liquids and Solids

Advanced Chemistry Chapter 10

Page 2: Adv chem chapt 10

SectionsIntermolecular Forces

Liquid state

Solid Structures

Metal Structures

Carbon and Silicon Networks

Page 3: Adv chem chapt 10

SectionsMolecular Solids

Ionic Solids

Vapor pressure and State Change

Phase Diagrams

Page 4: Adv chem chapt 10

States of Matter

When considering the three states of matter, properties of gases are strikingly different than solids and liquids. Liquids and solids share many similar characteristics

compressibility

density

intermolecular forces

Page 5: Adv chem chapt 10

States of Matter

H2O(s)H2O(l) ΔH°fus = 6.02 kj/mol

H2O(l)H2O(g) ΔH°vap = 40.7 kj/mol

Water densities:25°C and 1atm .99707g/cm3

25°C and 1065 atm 1.046g/cm3

400°C and 1atm 3.26x10-4 g/cm3

400°C and 242 atm .157g/cm3

Page 6: Adv chem chapt 10

Intermolecular Forces

10.1

Page 7: Adv chem chapt 10

Intermolecular Forces

Electrons shared within the molecule are called intramolecular bonding.

In the condensed states of matter the attraction between molecules are called intermolecular forces.

Page 8: Adv chem chapt 10

Intermolecular Forces

It is important to realize that when a molecule changes state, the molecule stays intact. The changes in state are due to the change in forces surrounding the molecule not from changes within the molecule.

40.7kj needed to vaporize water934kj to break the O-H bond

Page 9: Adv chem chapt 10

Dipole–Dipole Forces

Dipole-dipole forces occur when polar molecule (molecules with dipole moments) electrostatically attract each other by lining up the positive and negative ends of the dipoles.

Dipole-dipole forces are about 1% as strong as a covalent or ionic bond and rapidly become weaker when distances between the dipoles increases. The distances in a gas make these attractions relatively unimportant

Page 10: Adv chem chapt 10

Dipole-Dipole Forces

In a condensed state, molecules line up dipoles to minimize repulsions and maximize attractions.

Page 11: Adv chem chapt 10

Dipole-Dipole Forces

Some dipole-dipole forces are unusually strong. These usually form between H and another very electronegative atom.

These are stronger due to the high polarity of the bond and the closeness of the dipoles between the atoms.These strong attractions have a

strong impact on melting points and boiling points.

Page 12: Adv chem chapt 10

Boiling Points of Covalent Hydrides

Page 13: Adv chem chapt 10

Hydrogen bonds

Hydrogen bonds are the strongest in the smallest and lightest of the covalent molecules. This is primarily due to two factors:

large difference in electronegativities

small size of the atoms allows for close dipole interactions.

Page 14: Adv chem chapt 10

Hydrogen bonds

Page 15: Adv chem chapt 10

Hydrogen Bonds and Organics

Methanol (CH3OH) and ethanol (CH3CH2OH) have much higher boiling points than would be expected from their molar masses because of the O-H bonds that produce hydrogen bonding.

Page 16: Adv chem chapt 10

London Dispersion Forces

Even without dipoles, molecules exert forces on each other.

The forces that exist among noble gas atoms and nonpolar molecules are called London dispersion forces.

Page 17: Adv chem chapt 10

London Dispersion Forces

Usually it is assumed that electron dispersion is uniform throughout the molecule, but this is not always the case.

Since the movements of the electrons around the nucleus are somewhat random, a momentary nonsymmetrical electron distribution can develop that creates a temporary dipolar arrangement of charge.

Page 18: Adv chem chapt 10

London Dispersion Forces

This temporary change in polarity can, in turn, temporary change the distribution of the neighboring molecule.

This phenomenon leads to an inter-atomic attraction that is relatively weak and short-lived, but can be significant in larger atoms at lower temperatures.larger atoms have more electrons and

increases the probability of a temporary dipole.

Page 19: Adv chem chapt 10

London Dispersion Forces

Page 20: Adv chem chapt 10

London Dispersion Forces

Polarizability is the ease at which an electron cloud can be distorted into a temporary dipole.

large atoms have a larger polarizability than smaller atoms

This also applies to molecules like H2, CH4, CCl4 and CO2; smaller molecules, but nonpolar.

Page 21: Adv chem chapt 10

The Liquid State10.2

Page 22: Adv chem chapt 10

Liquid Characteristics

lack of rigidity

low compressibility

high density

rounded droplets

capillary action

viscosity

Page 23: Adv chem chapt 10

Rounded Droplets

Occur due to the intermolecular forces of the liquid. The liquid molecules are subject to attraction from the side and from below, so liquid tends to form a shape with the minimum surface area – sphere.

The resistance of a liquid to increase surface area is from the energy that it takes to overcome intermolecular forces. This resistance is called surface tension.

Page 24: Adv chem chapt 10

Rounded Droplets

Molecules that are polar and have stronger intermolecular forces have stronger surface tensions.

Page 25: Adv chem chapt 10

Surface Tension

Page 26: Adv chem chapt 10

Capillary Action

Capillary action is the spontaneous rising of a liquid in a narrow tube. This action is due to two forcescohesive forces- the intermolecular

forces among the molecules.adhesive forces – the attractive

forces between the liquid and the container.

Page 27: Adv chem chapt 10

Adhesive forces

Adhesive forces happen when bonds within the container have polar bondsFor example: glass has O atoms that

carry a partial negative charge that attracts the partial positive charge of the hydrogen in water. This balance between the strong cohesive forces and the strong adhesive forces produce a meniscus.

Page 28: Adv chem chapt 10

Adhesive forces

A nonpolar substance, such as mercury, has a convex meniscus because the cohesive forces are stronger than the adhesive forces.

Page 29: Adv chem chapt 10

Meniscus: Water vs. Mercury

Page 30: Adv chem chapt 10

ViscosityViscosity is a fluids resistance to flow.

liquids with strong cohesive forces tend to be highly viscous. Example: glycerol is highly viscous

because of its ability to create hydrogen bonds.

Page 31: Adv chem chapt 10

Viscosity

Molecular complexity also can affect viscosity because they can become entangled in each other.Example: Gasoline has carbon chains

from 3-8C long and is nonviscous. Grease is 20-25C long and is very viscous.

Page 32: Adv chem chapt 10

Introduction to Structures and Types of

Solids10.3

Page 33: Adv chem chapt 10

Types of Solids

Crystalline solids

Amorphous solids

Page 34: Adv chem chapt 10

Crystalline Solids

Crystalline solids have a regular arrangement of components at a microscopic level and produce beautiful, characteristic shapes of crystals:

Page 35: Adv chem chapt 10

Crystalline Solids

The positions of components are usually represented by a lattice.

lattice is a three dimensional system of units repeating in a pattern. The smallest repeating unit of the lattice is called the unit cell.

Page 36: Adv chem chapt 10

Three types of Crystalline Solids

Page 37: Adv chem chapt 10

Amorphous Solids

Amorphous solids have considerable disorder in their structures.

Example: Common glass looks like a solution frozen in place. It has a rigid shape but a great deal of disorder within its structure.

Page 38: Adv chem chapt 10

X-ray Analysis of Solids

The structures of crystalline solids are commonly determine by X-ray diffraction.

This type of diffraction occurs when beams of light are scattered as they go through spaces between substances. Light scatters when the size of the spaces are similar to the wavelength of light.

Page 39: Adv chem chapt 10

X-ray Analysis of Solids

Page 40: Adv chem chapt 10

X-ray Analysis of Solids

A single wavelength is directed at the crystal and a diffraction pattern is obtained. The diffraction pattern is a series of light and dark areas on a photographic plate from constructive and destructive interference from waves of light.

The diffraction pattern can then be used to determine the interatomic spacings.

Page 41: Adv chem chapt 10

X-ray Analysis of Solids

A diffractometer is a computer-controlled instrument used for carrying out the X-ray analysis of crystalsIt rotates the crystal with respect to

the X-ray beam and collects the data produced by the scattering. The techniques have been refined to the point that very complex structures can be determined, such as large biological enzymes.

Page 42: Adv chem chapt 10

X-ray Analysis of Solids

The Bragg equation combines trigonometry and physics to determine the atomic spaces between crystals:

nλ = 2d sin θ

d is the distance between atoms and θ is the angle of incidence and reflection of the light. n is an integer, most commonly 1. (n is usually given)

Page 43: Adv chem chapt 10

X-ray Analysis of Solids

Page 44: Adv chem chapt 10

Example Problem

X-rays of wavelength 1.54 Â were used to analyze an aluminum crystal. A reflection was produced at θ = 19.3°. Assuming n=1, calculate the distance d between the planes of atoms producing this reflection

2.33 Á

Page 45: Adv chem chapt 10

Types of Solids

Ionic solidsionic solids are made of ions

Molecular solidsMolecular solids have small units of

covalently bonded molecules.

Atomic solidsAtomic solids are made of elements such

as carbon (graphite, diamond and the fullerenes), boron, silicon, and all metals.

Page 46: Adv chem chapt 10

Types of Solids

Page 47: Adv chem chapt 10

Atomic SolidsAtomic solids are broken down into

subgroups depending on the bond that exists in the solid:

Metallic solidsHas delocalized nondirectional covalent

bonding.

Network solidsatoms bond with strong directional

covalent bonding that lead to giant molecules and networks

Page 48: Adv chem chapt 10

Atomic SolidsGroup 8A solidsnoble gases are attracted to each other

with London dispersion forces.

Page 49: Adv chem chapt 10

Classification of Solids

Page 50: Adv chem chapt 10

Structure and Bonding in Metals

10.4

Page 51: Adv chem chapt 10

Metal Characteristics

Most of the properties that we see in metals is due to the nondirectional covalent bonding found in metal crystals.

High thermal conductivity

Electrical conductivity

Malleability

Ductility

Page 52: Adv chem chapt 10

Metallic Crystals

Metallic crystals can be pictured as containing spherical atoms packed together that can be bonded to each other equally in all directions.

This arrangement is called closest packing.

Page 53: Adv chem chapt 10

Closest Packing

The spheres pack in layers. Each sphere is surrounded by six others. These layers do not lie directly over those in the first layer, instead they fill the indentations of the layer below. The third layer is in the same position as the first. This is called aba arrangement.

Page 54: Adv chem chapt 10

Closest Packing

The aba arrangement has the hexagonal unit cell and the resulting structure is called the hexagonal closest packed (hcp) structure.

The abc arrangement has a face-centered cubic unit cell and the resulting structure is called the cubic closest packed (ccp) structure. This has a repeating vertical placement every fourth layer.

Page 55: Adv chem chapt 10

Closest Packing

Page 56: Adv chem chapt 10

Closest Packing: Hexagonal

Page 57: Adv chem chapt 10

Closest Packed: Cubic

Page 58: Adv chem chapt 10

Closest Packing

Knowing the net number of atoms in a particular unit cell is important for many applications involving solids.

Page 59: Adv chem chapt 10

Closest Packing

Example: A face centered cube (unit cell) is defined by the centers of the spheres on the cube’s corners. Therefore 8 cubes share a given corner sphere, so 1/8 of this sphere lies inside the unit cell. (8 corners x 1/8 sphere = 1sphere). The sphere at the center of each face is shared by two cubes. (6 faces x ½ sphere = 3 spheres). The total number of spheres for a face centered cube is 4.

Page 60: Adv chem chapt 10

Closest Packing

Face – Centered Cubic Unit Cell

Page 61: Adv chem chapt 10

Cubic Substances

Metals that form cubic closest packed solids are:

aluminum

iron

copper

cobalt

nickel

Page 62: Adv chem chapt 10

Hexagonal Substances

Metals that form hexagonal closest packed solids are:

magnesium

zinc

Page 63: Adv chem chapt 10

Other Metal Solids

Calcium and certain other metals can crystallize in either cubic or hexagonal solids.

Some metals, including many alkali metals, have structures that are characterized by a body-centered cubic (bcc) unit cell. In this structure, each sphere has 8 neighbors.

Page 64: Adv chem chapt 10

Example Problem

Silver crystallizes in a cubic closest packed structure. The radius of a silver atom is 144pm. Calculate the density of solid silver?

10.6 g/cm3

Page 65: Adv chem chapt 10

Bonding Models for Metals

In order to determine bonding for metals, one must account for the typical properties: durable, high melting point, malleable, ductile, and efficient in uniform conduction of heat and electricity in all directions.

These characteristics indicate that the bonds are strong and nondirectional. In other words, it is not easy to separate metal atoms but easy to move them.

Page 66: Adv chem chapt 10

Electron Sea Model

Metal cations ‘swim’ in a sea of valence electrons that are mobile and shared.

This accounts for conduction and malleability and ductility.

Page 67: Adv chem chapt 10

Electron Sea Model

Page 68: Adv chem chapt 10

Band Model (MO Model)

In this model, the electrons are assumed to travel around the metal crystal in molecular orbitals formed from the valence atomic orbitals of the metal atoms.

When metals atoms interact, the large number of resulting molecular orbitals become more closely spaced and finally form a virtual continuum of levels, called bands.

Page 69: Adv chem chapt 10

Band Model (MO Model)

Page 70: Adv chem chapt 10

Band Model

The electrons in partially filled MO’s are mobile. These conduction electrons are free to travel throughout the metal crystal. The MO occupied by these conducting electrons are called conduction bands.

Page 71: Adv chem chapt 10

Band Model

Page 72: Adv chem chapt 10

Metal Alloys

An alloy is best defined as a substance that contains a mixture of elements and has metallic properties. There are two types of alloys:

Substitutional alloy– some of the host metal atoms are replaced by other metal atoms of similar size.

Interstitial alloy – is formed when some of the interstices (holes) in the closest packed lattice are occupied by smaller atoms.

Page 73: Adv chem chapt 10

Metal Alloys

Page 74: Adv chem chapt 10

Substitutional Alloys

Example: brass: 1/3 of copper metal atoms are replaced by zinc atoms

Sterling silver- 93% silver and 7% copper.

Pewter- 85% tin, 7% copper, 6% bismuth and 2% antimony.

Plumbers solder – 95% tin and 5% antimony

Page 75: Adv chem chapt 10

Interstitial Alloy

Example: Steel contains carbon atoms in the holes of an iron crystal. The presence of the interstitial atoms changes the properties of the host metal. Iron is relatively soft, ductile and malleable, but when carbon (which forms directional bonds), is introduced into the crystal, it makes the iron bonds stronger and less ductile.

Page 76: Adv chem chapt 10

Interstitial Alloy

The amount of carbon directly affects the properties of steel:

Mild steels- contains less than .2% carbon: nails chains and cables.

Medium steels- contain .2-.6% carbon: rails and structural steel

High-carbon steel – .6-1.5% carbon: springs, tools and cutlery.

Page 77: Adv chem chapt 10

Mixed AlloysSome steels contain elements in addition

to iron and carbon. These are called alloy steels and are viewed as being mixed interstitial and substitutional alloys.

Bicycle frames are usually constructed from a wide variety of alloy steels.

Page 78: Adv chem chapt 10

Carbon and Silicon Network Atomic Solids

10.5

Page 79: Adv chem chapt 10

Network Solids

Many atomic solids contain strong directional covalent bonds to form a solid that might be viewed as a “giant molecule.” These materials are typically brittle and do not efficiently conduct heat and electricity. Two examples of these network solids are carbon and silicon.

Page 80: Adv chem chapt 10

CarbonTwo most common forms of carbon are

diamond and graphite. They are typical network solids.

Diamond is the hardest naturally occurring substance.

Graphite is slippery, black and a conductor.

Page 81: Adv chem chapt 10

DiamondEach carbon is surrounded by a tetrahedral

arrangement of other carbon atoms to form a large molecule. Diamond is an insulator not a conductor. Each carbon is sp3 hybridized with localized bonding and therefore does not conduct.

Diamonds are often used for industrial cutting implements.

The application of 150,000 atm at 2800°C can break graphite bonds and rearrangement into a diamond structure.

Page 82: Adv chem chapt 10

Graphite

The structure of graphite is based on layers of carbon atoms arranged in fused 6 C rings. The unhybridized p orbitals allow for delocalized electrons and therefore conductivity.

Graphite is used as a industrial lubricant. Because graphite has strong bonds within the layers and weak bonding between the layer, the layers slide past one another readily.

Page 83: Adv chem chapt 10

Carbon

Page 84: Adv chem chapt 10

Carbon: Graphite layers

Page 85: Adv chem chapt 10

Silicon

Silicon is an important constituent of the compounds that make up the earth’s crust. Silicon is to geology what carbon is to biology and is fundamental to most rocks, sands and soils found in the earth’s crust.

Carbon compounds typically have long strings of C-C bonds

Silicon compounds typically involve chains of Si-O bonds.

Page 86: Adv chem chapt 10

SilicaThe fundamental

silicon-oxygen compound is silica, which has the empirical formula SiO2. The structure that is formed is based on a network of SiO4 tetrahedra with shared oxygen atoms rather than smaller SiO2 units.

Page 87: Adv chem chapt 10

SilicaWhen silica is heated

above its melting point (1600°c) and cooled rapidly, an amorphous solid called glass results. Glass has a lot of disorder as opposed to the crystalline nature of quartz. Glass, also homogeneous, more closely resembles a very viscous solution than it does a crystalline solid.

Page 88: Adv chem chapt 10

GlassThe properties of glass can vary greatly

depending on the additives.

Common glass results when substances like Na2CO3 are added to the silica melt.

B2O3 produce borosilicate glass which does not expand and contract during large temperature changes. (Pyrex)

K2O produces especially hard glass that can be ground into shapes for lenses and contacts.

Page 89: Adv chem chapt 10

Glass

Page 90: Adv chem chapt 10

Silicates

Compounds closely related to silica and found in most rocks, soils and clays are the silicates. Like silica, the silicates are based on interconnected SiO4 tetrahedra, but instead of a O/Si ratio of 2:1, the ratio is typically higher. This higher ratio tends to make silicon-oxygen anions.

Page 91: Adv chem chapt 10

Silicates

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Silicates

Ceramics are typically made from clays (which contain silicates) and hardened by firing at high temperatures. They tend to be strong, brittle and heat and chemical resistant.

Ceramic is heterogeneous and contain two phases: minute crystals of silicates that are suspended in a glassy cement.

Page 93: Adv chem chapt 10

ClaysClay comes from the weathering

of feldspar, an Aluminosilicate (Na2O/K2OAl2O36SiO2). This weathering produces kaolinite, that consists of tiny thin platelets of Al2Si2O5(OH)4. When dry these platelets cling together and lock into place; when wet they can slide over one another. During firing, these platelets bind and form a glass.

Page 94: Adv chem chapt 10

CeramicsCeramics constitute one of the most important

classes of ‘high-tech” materials. Their stability at high temperatures and resistance to corrosion, make them an obvious choice for constructing jet and car engines.

Organoceramics are taking form by the addition of organic polymers to ceramics. This reduces some of the brittle nature of ceramics and allows them to be used for things such as flexible superconducting wire, microelectronic devices, prosthetic devices and artificial bones.

Page 95: Adv chem chapt 10

Semiconductors

Elemental silicon has the same structure as diamond. The structure is different in that the energy gap between filled and empty MO’s is not as large and electrons can delocalize and make silicon a semi-conductor. At higher temperatures, more electrons get excited in the conduction bands and the conductivity of silicon increases.

Page 96: Adv chem chapt 10

N-type Semiconductor

When small fraction of silicon atoms are replaced by arsenic atoms (one more valence electron), extra electrons become available for conduction and produce an n-type semi-conductor. These can conduct an electric current.

Page 97: Adv chem chapt 10

P-type Semiconductor

When small fraction of silicon atoms are replaced by boron atoms (one less valence electron), an electron ‘vacancy’ is made. As electrons move, the fill the ‘hole’ and make a new one. This movement of electrons can therefore carry a current. This type of conductor (less electrons) is called a p-type semiconductor.

Page 98: Adv chem chapt 10

Energy Level Diagrams for N-type and P-type Semiconductors.

Page 99: Adv chem chapt 10

P-N Junction

Most important applications of semiconductors involve connection of a p-type and an n-type to form a p-n junction.

The red dots represent excess electrons in the n-type semiconductor and the white circles represent holes (electron vacancies.

Page 100: Adv chem chapt 10

P-N Junction

At the junction a small number of electrons migrate from the n-type region into the p-type region. The effect of these migrations is to place a negative charge on the p-type region and a positive charge on the n-type region.

Page 101: Adv chem chapt 10

P-N Junction

This charge buildup, called the contact potential or junction potential, prevents further migration of electrons. This transfer of electrons is therefore a ‘one-way’ transfer and under an external battery source will allow flow of electrons from the n to the p type regions.

Page 102: Adv chem chapt 10

P-N Junction

When current is opposed it is said to be under reverse bias. When current flows easily, the junction is said to be under forward bias.

A p-n junction is a good rectifier, a device that produces a pulsating direct current from an alternating current.

Page 103: Adv chem chapt 10

P-N Junction

When placed in a circuit where the current is constantly reversing, a p-n junction only transmits current under forward bias. Radios, computers and other electronic devices all use this rectifiers. This p-n junction revolutionized electronics.

Page 104: Adv chem chapt 10

Molecular Solids10.6

Page 105: Adv chem chapt 10

Network Solids

Sometimes network solids can be considered to be one giant molecule or have large discrete molecular units in a lattice-type position. These molecules have strong bonds within the molecules but relatively weak between the molecules.

Common examples: Ice, dry ice (solid carbon dioxide), Sulfur (S8), Phosphorus (P4)

Page 106: Adv chem chapt 10

Network Solids

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Network Solids

When molecules do have dipole moments, their intermolecular forces are significantly greater, especially when hydrogen bonding is possible.

Water not only has polar bonds, a dipole moment, has hydrogen bonds, but it also can have a total of four hydrogens associated with every oxygen atom.

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Ionic Solids10.7

Page 109: Adv chem chapt 10

Ionic Solids

Ionic solids are stable, high melting substances held together by the strong electrostatic forces that exist between oppositely charged ions.

Page 110: Adv chem chapt 10

Ionic SolidsMost binary ionic solids can be explained

by the closest packing of spheres. Typically the larger ions, usually anions, are packed in one of the closest packed arrangements (hcp and ccp).

The smaller cations fit into the holes among the closest packed anions. This packing maximizes the electrostatic attractions among oppositely charged ions and minimizes the repulsion of like charges.

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Ionic SolidsThere are three

types of holes in closest packed structures:

1.Trigonal holes are formed by three spheres in the same layer

Page 112: Adv chem chapt 10

Ionic SolidsThere are three

types of holes in closest packed structures:

2.Tetrahedral holes are formed when a sphere sits in the dimple of three spheres in an adjacent layer.

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Ionic SolidsThere are three

types of holes in closest packed structures:

3.Octahedral holes are formed between two sets of three spheres in adjoining layers of the closest packed structures.

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Ionic Solids

The holes increase in size in the order:

trigonal < tetrahedral < octahedral

The trigonal holes are so small that they are never occupied in binary ionic compounds. Tetrahedral and octahedral holes are occupied if the relative sizes of the ions allow.

Page 115: Adv chem chapt 10

Ionic SolidsExample: Zinc Sulfide (ZnS) creates a ccp

structure. The Zn2+ has a radius of 70pm and the S2- ion has an ionic radius of 180pm. There are 4 spheres (atoms/anions) in a face-centered cubic unit cell and 8 tetrahedral holes. So only half of the holes in the ccp unit are filled with cations.

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Ionic SolidsExample: Sodium chloride can be described in

terms of a ccp structure. Na+ resides in octahedral holes. The locations of the octahedral holes in the face-centered cubic unit is marked by X. The number of spheres (anions) in the structure is the same number of octahedral holes. Since NaCl is a 1:1 binary compound. All octahedral holes are used.

Page 117: Adv chem chapt 10

Example Problem

Determine the net number of Na+ and Cl- ions in the sodium chloride unit cell.

4 Na+ and 4 Cl-

Page 118: Adv chem chapt 10

Example Problem

Classify each of the following substances according to the type of solid it forms:gold

carbon dioxide

lithium fluoride

krypton

metallic

molecular

ionic

8a

Page 119: Adv chem chapt 10

Types and Properties of Solids

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Vapor Pressure and Changes of

State10.8

Page 121: Adv chem chapt 10

Vaporization

Vaporization, or evaporation, is the process of liquid molecules escaping the liquid’s surface and forming a gas.

Vaporization is endothermic because energy is required to overcome the relatively strong intermolecular forces in the liquid. Water has strong intermolecular forces and

this increases the energy required to vaporize. Also making it a great coolant.

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Vaporization

The energy required to vaporize 1 mole of liquid at 1 atm is called the heat of vaporization or the enthalpy of vaporization.The symbol for this is ΔHvap.

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Vapor Pressure

Condensation is the process by which vapor molecules re-form a liquid.

The evaporation process occurs at a constant rate at a given temperature, and once an equilibrium has been reached, the rate of condensation will equal the rate of evaporation.

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Vapor PressureMolecules in a

given system are constantly escaping from and entering the liquid at high rate. However, there is not net change because the two opposite processes just balance each other.

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Rates of Condensation and Evaporation.

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Vapor Pressure

The pressure of the vapor present at equilibrium is called the equilibrium vapor pressure, or more commonly, the vapor pressure of the liquid.

A simple barometer can measure the vapor pressure of a liquid.

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Vapor PressureLiquid is injected at the bottom of the tube of

mercury and floats to the surface. A portion of the liquid evaporates at the top of the column, producing a vapor whose pressure pushes some mercury out of the tube.

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Vapor PressureWhen the system reaches equilibrium,

the vapor pressure can be determined from the change in the height of the mercury column

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Vapor PressurePatmosphere = Pvapor + PHg column

Pvapor = Patmosphere - Phg column

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Vapor Pressure

The vapor pressure of liquids vary widely. Liquids with high vapor pressures are said to be volatile. They evaporate rapidly in an open dish.

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Vapor Pressure

The vapor pressure of a liquid is principally determined by the size of the intermolecular forces in the liquid.Liquids with strong molecular forces

have relatively low vapor pressures because it takes so much energy for the molecules to escape.

In general, substances with large molar masses have relatively low vapor pressures due of large dispersion forces.

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Vapor Pressure

Vapor pressure increases significantly with temperature. In order to break intermolecular forces,

a sufficient amount of kinetic energy is needed.

As temperature of the liquid increases, so does kinetic energy of the liquid.

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Vapor Pressure

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Vapor Pressure of Water

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Vapor Pressure

The nature of the temperature, vapor pressure relationship is quadratic. Pvap vs. 1/T (Kelvin) gives a direct relationship.

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Vapor Pressure

Vapor pressure equation:

R is the universal gas constant (8.3145 J/K), and C is a constant characteristic of a given liquid (y=intercept). In means natural logarithm.

ln(Pvap ) = −ΔHvap

R

1

T

⎝ ⎜

⎠ ⎟+C

Page 137: Adv chem chapt 10

Example Problem

Using the graph, determine whether water or diethyl ether has the larger enthalpy of vaporization.

Ether has the smaller slope therefore smaller ΔHvap

Page 138: Adv chem chapt 10

Example Problem

The vapor pressure of water at 25°C is 23.8 torr, and the heat of vaporization of water at 25°C is 43.9 kj/mol. Calculate the vapor pressure of water at 50°C.

93.7 torr

Page 139: Adv chem chapt 10

Sublimation

Like liquids, solids have vapor pressures. When a solid sublimes, it goes directly from the solid to the gaseous state without passing through the liquid state.

Example: Dry Ice.

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Changes of State

Typically when a solid is heated, it will form a liquid and then boil to form a vapor. This process can be represented by a heating curve.

Temperature vs. time when energy is added a constant rate.

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Heating Curve

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Heating Curve

The plateaus in the heating curve represent the positions of phase change.

At the melting point, the temperature remains constant until the solid has completely changed to liquid.

At the boiling point the temperature remains constant as the added energy is used to vaporize the liquid

Page 143: Adv chem chapt 10

Heating CurveThe energy change that occurs at the

melting point when a solid melts is called heat of fusion or enthalpy of fusion.Note that changes of state are physical

changes, although intermolecular forces have been broken, no chemical bonds have been broken.

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Enthalpy of Fusions and Melting Points

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Melting and Boiling

The melting and boiling points for a substance are determined by the vapor pressure of the solid and liquid states.

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Melting and Boiling

At 0°C the vapor pressure of ice is less than that of liquid. Vapor pressure of ice increases more rapidly than water.

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Melting and Boiling

A point is reached when the liquid and solids have identical vapor pressures. This is the melting point.

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Freezing Point

At a temperature at which the vapor pressure of the solid is greater than that of the liquid, the solid would sublime and the vapor would be added to the water.

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Freezing Point

At a temperature at which the vapor pressure of the solid is less than that of the liquid, the liquid would evaporate and the vapor would be added to the ice.

Page 150: Adv chem chapt 10

Freezing Point

At a temperature at which the vapor pressures of the solid and liquid are identical, the vapor is in equilibrium. This is the freezing point of water.

Page 151: Adv chem chapt 10

Melting Point and Boiling Point

The normal melting point of a liquid is the temperature at which the solid and liquid states have the same vapor pressure under conditions where the total pressure is 1 atmosphere.

The normal boiling point of a liquid is the temperature at which the vapor pressure of the liquid is exactly 1 atmosphere.

Page 152: Adv chem chapt 10

Supercooled and Superheated

Changes of state do not always occur exactly at the boiling point or melting point.

Water can be supercooled below 0°C at 1 atm and remain in the liquid state. At some point the correct ordering of molecules occurs and ice forms, releasing energy in the exothermic process and bringing the temperature back up to the melting point.

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Supercooled and Superheated

Page 154: Adv chem chapt 10

Supercooled and Superheated

Changes of state do not always occur exactly at the boiling point or melting point.

A liquid can also be superheated, or raised to temperatures above its boiling point, especially if it is heated rapidly. Boiling requires high-energy molecules to gather in the same vicinity for bubble formation. This may not happen at the boiling point.

Page 155: Adv chem chapt 10

Supercooled and Superheated

Once a bubble does form, when a liquid is superheated, its internal pressure is greater than the atmospheric pressure. This bubble can burst before rising to the surface, blowing the surrounding liquid out of the container. This is called bumping and is a common experimental problem.

Page 156: Adv chem chapt 10

Supercooled and Superheated

Boiling chips are often added to prevent bumping. These are bits of porous ceramic material containing trapped air that escapes on heating, forming tiny bubbles that act as ‘starters’ for the vapor bubble formation. This allows for smooth onset of boiling.

Page 157: Adv chem chapt 10

Phase Diagrams10.9

Page 158: Adv chem chapt 10

Phase Diagram

A phase diagram is a convenient way of representing the phases of a substance as a function of temperature and pressure. It shows which state exists at a given temperature and pressure.

Conditions for these phase diagrams are assumed to be a closed system and is plotted as temperature vs pressure.

Page 159: Adv chem chapt 10

Phase Diagram

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Phase Diagram

The solid/liquid boundary has a negative slope. Melting point of ice decreases as

external pressure increases. This is different for most substances

other than water because the density of ice is less than that of liquid water at the melting point.

Page 161: Adv chem chapt 10

Boiling Points of Water vs. Pressure

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Example 1

Pressure is 1 atm. Water moves through the changes of state according to the vapor pressure at the corresponding temperatures.

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Example 2

Pressure is 2 torr. Water will sublime at -10°C. This is when the vapor pressure of the ice is equal to the external pressure of 2 torr. Vapor pressure of liquid water is always greater than 2 torr and therefore will not form.

Page 164: Adv chem chapt 10

Example 3Pressure is 4.58 torr.

When temperature reaches .01°C (273.16K), water reaches the triple point. Solid and liquid water have identical vapor pressures and all three states of water exist. This is the only condition in a closed system that allows this.

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Example 4

Pressure is 225 atm. Liquid water can be present at this temperature because of the high external pressure. As temperature increases, liquid gradually turns to vapor, but goes through a ‘fluid’ region.

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Example 4

The fluid region is neither true liquid or vapor. This unusual behavior occurs because the conditions are beyond the critical point for water.

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Critical PointThe critical temperature can be defined

as the temperature above which the vapor cannot be liquefied no matter what pressure is applied.

The critical pressure is the pressure required to produce liquefaction at the critical temperature

Together, the critical temperature and critical pressure define at the critical point.

Page 168: Adv chem chapt 10

Critical PointThe critical point for water is 374°C

and 218 atm. Anything beyond this point, involves the intermediate “fluid” region.

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Phase Diagrams

The phase diagram for CO2 shows the liquid state does not exist at a pressure of 1 atm. The solid/liquid line has a positive slope, since the density of solid CO2 is greater than that of liquid CO2

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THE END!!


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