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Liquids and Solids

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Title: Liquids and Solids


1
Liquids and Solids
  • Chapter 13

2
Solids, Liquids, and Gases
  • Solids liquids are condensed states
  • atoms, ions, molecules are close to one another
  • highly incompressible
  • Liquids gases are fluids
  • easily flow
  • Intermolecular attractions in liquids solids
    are strong
  • Look at Table 13-1 for a general description of
    characterisitics

3
Kinetic-Molecular Description of Liquids and
Solids
  • When a gaseous sample is cooled or compressed the
    rapid, random motion of the molecules decrease.
    The attraction between molecules becomes
    significant. When the attractive forces overcome
    the reduced kinetic energies, condensation occurs
    (or the gas turns to a liquid).
  • In the liquid phase the particles are close.
    Very little space is unoccupied (discuss).
  • The particles, however, still have sufficient
    KEs to partially overcome the attractive forces.
    Therefore, liquids are considered fluids and can
    take the shape of a container.

4
Kinetic-Molecular Description of Liquids Solids
  • Liquids that diffuse into one another are
    miscible (i.e. one liquid is soluble in the
    other)
  • Water and methanol/gasoline and motor oil
  • Immiscible liquid do not diffuse into one another
    (i.e. one liquid is not soluble in the other)
  • Water and hexane/water and gasoline

5
Kinetic-Molecular Description of Liquids Solids
  • Cooling the liquid lowers the KE even more.
    Shorter-range attractive force become important
    and the liquid solidifies. Particles in a solid
    cannot move freely past one another as they can
    in a liquid. This is why solids have definite
    shapes and volumes. Solids are essentially
    incompressible.
  • If diffusion occurs in solids, it is very slow.

6
Intermolecular Attractive Forces
  • Intermolecular attractive forces are the forces
    between individual particles of a substance.
  • Generally, these forces are very weak compared to
    intramolecular forces (e.g. covalent and ionic
    bonds)
  • Covalent bonding and attractive forces in H2O(l)
  • Important physical properties such as boiling
    points, vapor pressure, heat of vaporation,
    melting points, and heat of fusion depend on the
    strength of these intermolecular attractive
    forces.
  • If intermolecular attractive forces did not
    exist, solids and liquids would not exist (only
    gases)

7
Ion-Ion Interactions
  • The force of attraction between two charged
    particles can be determined from Coulombs Law
  • where q and q- are the charges on the particles
    and d is the distance between them.

8
Ion-Ion Interactions
  • The energy of attraction between charged
    particles is given by
  • The energy of attraction is large for ionic
    compounds due to the charged particles that are
    close together when substance is a solid.
  • The melting points for ionic compounds is
    relatively high.
  • For a given substance, the separation between
    particles in the solid is less than the
    separation in liquids.
  • Energy of attraction is greater in the solid
    phase (generally)

9
Ion-Ion Interactions
  • Ionic compounds that possess multiply-charged
    ions (e.g. Al3 and O2-) usually have higher
    melting points than ionic compounds that posses
    singly-charged particles. Why (two reasons)?
  • Arrange the following ionic compounds in the
    expected order of increasing melting and boiling
    points.
  • NaF, CaO, CaF2

10
Dipole-Dipole Interactions
  • Permanent dipole-dipole interactions occur
    between polar covalent molecules because of the
    attraction between ?- and ? on different
    molecules.
  • Generally, these forces are not as strong as
    ion-ion interactions
  • Attraction between partial charges
  • Dipole-dipole forces vary as 1/d4 instead of 1/d2
  • Decrease faster

11
Dipole-Dipole Interactions
The partial positive charge on the hydrogen
atoms is attracted to the partial negative charge
on the nitrogen atoms. Note Dipole-dipole
interactions are dependent on temperature. Why?
12
Hydrogen Bonding
  • Hydrogen bonding is a special type of strong
    dipole-dipole interaction
  • Occurs between covalent molecules containing H
    and of the three small, highly electronegative
    elements-F, O, or N.
  • One molecule most possess a H atom attached to
    one of these highly electronegative atoms.
  • The other molecule most possess one these highly
    electronegative atoms.

13
Hydrogen Bonding
The partial negative charge of one molecule is
attracted to the partial positive charge of
another molecule. The small sizes of F, O, and N
and their high electronegativities concentrate
the electrons around these atoms.
14
Hydrogen Bonding
  • Typical hydrogen-bond energies are greater than
    dipole-dipole energies
  • 15-20 kJ/mol for hydrogen-bond energies
  • 4 kJ/mol for dipole-dipole energies
  • 400 kJ/mole for ion-ion interaction energies
  • Hydrogen bonding is responsible for the high
    boiling points of water and methanol.

15
Dispersion Forces
  • These are attractive forces that are present in
    all types of molecules.
  • Dispersion forces are weak in small molecules.
  • They are important at extremely small distances
    which vary as 1/d7.
  • They are the only attractive force present in
    symmetrical nonpolar substances such as Cl2 and
    monatomic species.

16
Dispersion Forces
  • Dispersion forces result from the attraction of a
    positively charged nucleus to the electron cloud
    of another atom in nearby molecules. As a
    result, temporary dipoles are induced in the
    neighboring atoms or molecules.
  • The magnitude of the temporary dipole increases
    with increasing size of the electron cloud (or
    size of the molecule). The larger electron cloud
    is more diffuse and easily distorted. Adjacent
    molecules are polarized by the adjacent nuclei.
    Polarizibility increases with increasing sizes of
    molecules.
  • Dispersion forces are, therefore, stronger for
    molecules that are larger or have more electrons.

17
Dispersion Forces for Argon
Dispersion forces can also exist between
cations/anions and polarizable atom or molecule.
Examine Figure 13-6.
18
Dispersion Forces
  • Some trends observed in increasing boiling points
    can largely be attributed to dispersion forces
    (Figure 13-5).
  • CH4, SiH4, GeH4, and SnH4
  • HCl, HBr, and HI
  • Understand Table 13-3.
  • Heat of vaporization measures the energy required
    to overcome attractive forces in the liquid.

19
The Liquid State
  • Viscosity - the resistance to flow of a liquid.
  • Generally, the higher the attractive forces in a
    liquid, the greater the viscosity.
  • Water versus honey or Karo syrup.
  • Pentane versus dodecane
  • Viscosity decreases with increasing temperature.
    Why?

20
The Liquid State
  • Surface Tension - measure of the inward forces
    that must be overcome to expand the surface area
    of a liquid.
  • Molecules at the surface are attracted unevenly.
  • Water bugs and floating razor blades (or needles)
  • Demo Razor blade or needle

21
Liquid State
  • Capillary action - ability of a liquid to rise or
    fall in a tube.
  • Cohesive forces forces holding a liquid
    together.
  • Adhesive force forces between a liquid and
    another surface
  • Capillary action
  • Capillary rise implies adhesive forces gt cohesive
    forces
  • Capillary fall implies cohesive forces gt adhesive
    forces
  • Water is attracted to a glass capillary tube due
    to attractive forces between the partial negative
    oxygens on the surface of the glass and the
    partial positive charges on the hydrogen atoms.

22
Liquid State
  • Capillary Action
  • The meniscus of water has a concave shape due to
    the strong adhesive forces between the water
    molecules and the glass graduated cylinder.
  • The meniscus of Hg has a convex shape because the
    cohesive forces are much stronger than the
    adhesive forces (Figure 13-9).

23
Liquid State
  • Evaporation process by which molecules escape
    from the surface of a liquid.
  • Only the molecules at the surface with sufficient
    KE will be able to escape the attractive forces
    present in the liquid. Therefore, the rate of
    evaporation is proportional to ________.

24
Liquid State
  • Evaporation
  • As the faster molecules leave the liquid, the
    flower molecules are left behind. What will this
    do to the temperature?
  • This process is termed as the cooling by
    evaporation.
  • DEMO Thermometer in acetone

25
Liquid State
  • Evaporation and condensation
  • In an open container/beaker, all the water that
    is present will eventually escape into the
    gaseous phase (Figure 13-10).
  • What if the beaker is sealed? What will happen?
    After molecules enter the gas phase they may be
    recaptured by the liquid by collisions. This
    process is called _______. At some point in
    time, the amount of gaseous molecule leaving the
    gaseous phase will equal the amount reentering
    the liquid phase. This is termed as dynamic
    equilibrium.

26
Liquid State
  • Vapor pressure the partial pressure of vapor
    molecules above the surface of a liquid at
    equilibrium.
  • Vapor pressure increases with temperature. Why?
    Look at Figure 13-13.
  • Vapor pressure decreases with increasing
    attractive forces. Why? Look at Table 13-4.
  • Hydrogen bonding, dipole-dipole, and dispersion
    forces.
  • DEMO H2O and ethyl ether (add H2O to ethyl
    ether)

27
Liquid State
  • As the temperature is increased, the vapor
    pressure increases until the liquid boils.
  • Boiling point temperature at which the vapor
    pressure equals the external pressure.
  • The boiling point of H2O is less in Rexburg.
    Why?
  • Normal boiling point temperature at which the
    vapor pressure of a liquid is equal to 1 atm.
  • Boiling point at 1 atm
  • What if the external pressure is lower over
    water?
  • DEMO Evacuate a flask filled with water

28
Liquid State
  • Distillation a method used to separate
    components in a solution based on differences in
    boiling point temperatures.
  • Separation of liquids in a solution
  • Purification of water (distilled water)
  • Separate impurities (e.g. ions) from tap water
  • Describe the basics of operation (Figure 13-14)
  • Of course, this can be related to vapor pressures.

29
The Liquid State
  • Heat transfer involving liquids
  • Specific heat or molar heat capacity of a liquid
    is the amount of heat that must be added to 1
    gram or 1 mole to raise the temperature by 1?C.
  • How much heat is released by 200 g of H2O as it
    cools from 85.0oC to 40.0oC? The specific heat
    of water is 4.184 J/goC.
  • Review in Chapter 1 if needed.

30
The Liquid State
  • The specific heat equation involves changing the
    temperature without a change in state. For a
    liquid, the temperature increases until the
    boiling point is acquired. The temperature
    remains at the boiling point temperature until
    all the liquid has been converted into the gas.
  • Boiling water is always 100?C at sea level
  • If the temperature is not increasing, what is all
    the heat/energy being used for when the liquid is
    boiling?
  • Boiling water on a hotplate or a stove

31
The Liquid State
  • Answer The heat is providing the energy
    necessary to break up the intermolecular
    attractive interactions present in the liquid.
  • Molar heat of vaporization amount of heat that
    must be added to one mole of the liquid at its
    boiling point to convert it to vapor
  • There is no change in temperature
  • How does heat of vaporization relate to
    intermolecular attractive forces and vapor
    pressure (Table 13-5)
  • How does this relate to the cooling effect of
    perspiration?

32
The Liquid State
  • Condensation is the reverse of vaporization/evapor
    ation.
  • Heat of condensation is the amount of heat that
    must be removed from a vapor to condense it.
  • Heat is released when the substance condenses.

33
Liquid State
  • Calculate the amount of heat necessary to convert
    125 grams of water at 25.0?C to steam at 100?C.
  • How many joules of energy must be absorbed by 500
    g of H2O at 50.0oC to convert it to steam at
    120oC? The molar heat of vaporization of water
    is 40.7 kJ/mol and the molar heat capacities of
    liquid water and steam are 75.3 J/mol oC and 36.4
    J/mol oC, respectively.
  • If 45.0 g of steam at 140oC is slowly bubbled
    into 450 g of water at 50.0oC in an insulated
    container, can all the steam be condensed?

34
Liquid State
  • Many trends in physical properties can be
    explained form the strength of intermolecular
    attractive forces in the liquid.
  • Table 13-6 (understand these trends based on
    intermolecular attractive forces)
  • Arrange the following substances in order of
    increasing boiling points.
  • C2H6, NH3, Ar, NaCl, AsH3
  • Discuss trends on Figure 13-5 (others as
    required)
  • Generally, if a group of molecules possess the
    same type of attractive forces, the boiling point
    increases with size/molecular weight of the
    compound.

35
The Clausius-Clapyron Equation
  • The equation relates the vapor pressure of
    liquids at different temperatures.
  • The vapor pressure is equal to 760 at the normal
    boiling point.
  • Appendix E and Table 13-5 produce some normal
    boiling point temperatures (measured at 1 atm).
    These values could be used in the equation above.
  • Also, the vapor pressure at the boiling point is
    equal to the atmospheric pressure

36
The Clausius-Clapyron Equation
  • At what temperature is the vapor pressure of
    water equal to the atmospheric pressure at sea
    level? Would the vapor pressure of boiling water
    in Rexburg be higher or lower than boiling water
    at sea level? Why?
  • In Rexburg, the normal atmospheric pressure is
    652 torr. At what temperature does water boil in
    Rexburg?
  • What will be the vapor pressure of ethyl alcohol
    at room temperature (298 K)?
  • Remember to use the appropriate R.

37
The Solid State
  • The melting point/freezing point of a substance
    is the temperature at which the solid and liquid
    phases coexist in equilibrium.
  • The normal melting point is the melting point at
    one atmosphere
  • Changes in pressures have very small effects on
    melting point

38
Heat Transfer Involving Solids
  • When heat is added to a solid the temperature
    increases until the melting point is acquired.
    Additional heat is required to convert the solid
    to a liquid (melting). Why? Heat that is added
    during the melting process does not increase the
    temperature. Temperature will rise after the
    solid is all converted to the liquid.

39
Heat Transfer Involving Solids
  • Molar heat of fusion (?Hfus kJ/mol) is the
    amount of heat required to melt one mole of a
    solid at its melting point. This can be
    converted to heat of fusion which is (kJ/g)
  • Heat of fusion depends on _________(Table 13-7)
  • Molar heat of solidification/crystallization is
    equal in magnitude (but opposite sign) to the
    molar heat of fusion.
  • 6.02 kJ is absorbed when 1 mole is melted and
    6.02 kJ is released when 1 mole is
    frozen/solidifies.

40
Heat Transfer Involving Solids
41
Heat Transfer Involving Solids
  • Calculate the amount of heat required to convert
    150.0 g of ice at -10.0oC to water at 40.0oC.
    The specific heat of ice is 2.09 J/goC
  • Calculate the amount of heat required to convert
    75.0 g of solid ethanol at 117.0?C to gaseous
    ethanol at 95.0?C.
  • Table 13-5, 13-7 and and Appendix E

42
Sublimation and Vapor Pressures of Solids
  • Sublimation is the process by which a solid forms
    a gas (vaporizes) without passing through the
    liquid phase.
  • Dry ice (CO2)
  • Deposition is the reverse process by which a
    vapor forms a solid without passing through the
    liquid phase.
  • Discussion with chemical vapor deposition
  • Note Solids have vapor pressures, but they are
    generally very small

43
Phase Diagrams (P versus T)
  • Phase diagrams illustrate a particular phase or
    state that is present under specific
    temperature-pressure conditions.
  • Temperature is on the y-axis and pressure is on
    the x-axis.
  • Using a phase diagram, changes in state can be
    determined when changing pressure and/or
    temperature.

44
Phase Diagrams (P versus T)
  • Phase boundaries
  • Line AC liquid and gas phases coexist at
    equilibrium
  • Line AB liquid and solid phases coexist at
    equilibrium
  • Line AD gas and solid phases coexist at
    equilibrium
  • Triple point (A) at this T and P all three
    phases coexist at equilibrium

45
Phase Diagrams (P versus T)
  • Notice the negative AB line slope. This is
    unique to H2O. What happens upon compressing a
    solid (up from point J)
  • Is there a pressure where sublimation could
    occur?
  • Travel a few other lines.

46
Phase Diagrams (P versus T)
  • When the temperature is increased at normal
    pressures the solid goes directly to the gas
    phase. At what pressure would the solid go
    through the liquid phase.
  • Notice the positive slope on the solid-liquid
    phase boundary. What does this mean?

47
Amorphous and Crystalline Solids
  • Amorphous solids do not possess well-ordered
    structures.
  • Some can also be characterized as glasses since
    they flow slowly.
  • Windows
  • Melting extend over a large range.
  • Rubber, plastics, and amorphous sulfur
  • Crystalline solids have well-defined structures
    consisting of repeating units.
  • Repeating unit can be observed upon shattering
    the crystal.
  • Possess distinct melting points.

48
Structures of Crystals
  • Crystals contain regularly repeating structures.
  • Unit cell is the smallest repeating unit of a
    crystal. A unit cell is the fundamental box that
    describes the arrangement of particles in a
    crystal. These unit cells are stacked in three
    dimensions to produce a crystal. The arrangement
    of these unit cells fit into one of seven crystal
    systems. (Table 13-9).
  • Crystals have the same symmetry as the unit cells
    since the crystals are built from multiple units
    of these cells.

49
Structures of Crystals
Look on page 513. Notice that the structures of
the unit cells are very similar to the actual
structure of the crystal. Why?
50
Structures of Crystals
  • Creating the crystal from the unit cells
  • Consider the corner of a unit cell as a lattice
    point. In three dimensions, this lattice point
    is shared by eight unit cells. If an object were
    present at this lattice point, it would be
    equally shared by all eight unit cells (1/8 in
    each). How many objects would be in each unit
    cell?
  • DEMO Use unit cell building blocks to
    illustrate.

51
Structures of Crystals
  • In a simple or primitive lattice structure
    (discussed previously), only the corners were
    occupied by objects. In other crystal types,
    objects may also occupy other positions in the
    unit cell.
  • Simple cubic (no additional objects)
  • Body-centered cubic (bcc) another object
    occupies the center of the unit cell
  • Face-centered cubic (fcc) another six object
    occupies the middle of each of the six square
    faces of the cube

52
Structures of Crystals
How many objects/atoms per unit cell for each
crystal type? Discuss Look at Figure 13-24.
53
Bonding in Solids
  • Categories of crystalline solids
  • Metallic solids
  • Ionic solids
  • Molecular solids
  • Covalent solids
  • Table 13-10 summarizes properties of each
    category type.

54
Metallic Solids
  • Positively charged nuclei are surrounded by a sea
    of delocalized valence electrons. This is the
    reason why most metals are good conductors.
  • The nuclei occupy lattice sites
  • Lattice types for metals
  • Body-centered cubic (bcc)
  • Face-centered cubic (fcc)
  • Hexagonal close-packed (hcp)
  • Examples Li, K, Ca, and Au

55
Metallic Solids
  • Obtaining the close-packed structures (fcc and
    hcp)
  • Hexagonal close packed structure has an ABA
    arrangement.
  • The different letters correspond to different
    planes (Figure 13-27a).
  • Face-centered cubic (or cubic close-packed)
    structure has an ABC arrangement.
  • Figure 13-27b
  • For the the close-packed structures approximately
    74 of the volume is occupied.
  • The body-centered cubic structures has much less
    of its volume occupied by metal spheres.

56
Metallic Solids
  • Manganese has a simple cubic unit cell. The
    atomic radius is 3.15 Å. What is the shortest
    distance between neighboring Mn atoms? How many
    nearest neighbors does each atoms have?
  • Nickel crystals are face-centered cubic. The
    radius of the nickel atom in the metal is 1.24Å.
    What is the distance between centers of the two
    closest Ni atoms. What is the length of the cell
    edge. How many nearest neighbors does each atoms
    have?
  • Calculate the density of metallic nickel.
    Determine the percentage of space that is
    occupied by the nickel atoms.

57
Metallic Solids
  • A group IVA element with a density of 11.35 g/cm3
    crystallizes in a face-centered cubic lattice
    whose unit cell edge length is 4.95 A. Calculate
    the elements atomic weight. What is the atomic
    radius of this element?

58
Ionic Solids
  • Most salts crystallize as ionic solids with ions
    occupying the unit cell. The most common example
    is sodium chloride, which has a face-centered
    cubic arrangement.
  • Many other salts that have the same charge on
    both the anion and cation have the same fcc
    arrangement (LiCl and MgO).
  • Even though the solid compound possesses charge,
    it does not conduct electricity. Why?

59
Ionic Solids
  • How many Cl- and Na ions are in the fcc unit
    cell? Remember, a sodium ion is in the center.
  • Illustrate models and look at 13-13 on demo CD.
  • Sodium iodide crystallizes in the fcc structure
    (like NaCl). The I- ion radius is 2.20 Å. The
    I- ions at the corners of the unit cell are in
    contact with those at the centers of the faces.
    Determine the length of the unit cell. Calculate
    the radius of the Na ion assuming anion-cation
    contact.

60
Molecular Solids
  • Molecules occupy the lattice positions of the
    unit cell.
  • There are covalent bond within the molecules but
    only intermolecular attractive forces between
    molecules. What are the types?
  • These solids tend to have lower melting points
    since the forces holding the molecules together
    are weaker.
  • Look at page 527 in book and 13-14 on demo CD.

61
Covalent Solids (network solids)
  • These can be considered giant molecules with the
    atom bond covalently in a crystalline network.
  • Structures are usually very hard with high
    melting points. Most are poor thermal and
    electrical conductors.
  • Examples Diamond, graphite, and quartz
  • What is the bonding in diamond (hydridization)
    and graphite?
  • 13-15 on demo. CD

62
Band Theory of Metals
  • Recall that the bonding in metals is due to
    delocalized, mobile electrons that belong to the
    solid as a whole.
  • Responsible for the conduction (electrical and
    thermal) of most metals.
  • Band theory of metals is used to explain
    properties of metals and other materials.
  • According to the MO theory, atomic orbitals
    overlap to produce a set of molecular orbitals.
    The number of generated molecular orbitals is
    equal to the number of overlapping atomic
    orbitals. There is a very large number of atomic
    orbitals in a metal!!!

63
Band Theory of Metals
  • In a Na metal, the 3s atomic orbitals overlap to
    produce a very large set of molecular orbitals
    that are very closely spaced in energy. These
    closely spaced orbitals are called a band of
    orbitals. Since there is only one electron in
    the 3s atomic orbital, the molecular orbitals are
    only half filled. Only a small amount of energy
    is needed for the highest energy electrons in the
    3s band to jump into a vacant orbital at a
    slightly higher energy.
  • As a result, electrons will flow with an applied
    field.

64
Band Theory of Metals
What if the 3s band is filled? In the Group IIA
metals, the 3s band is filled, but the metals
still conduct.
65
Band Theory of Metals
  • For Mg, the 3s and 3p band overlap since there is
    a range of energies for the molecular orbitals.
  • Without this overlap Mg metal would not conduct.
  • The highest energy electrons are able to move
    into the vacant orbitals in the 3p band.

66
Band Theory of Metals
  • Why dont some materials conduct electricity?
  • The highest energy electrons in insulators occupy
    filled bands of molecular orbitals that are well
    separated from the lowest empty band.
  • For semiconductors, the filled bands are only
    slightly below the empty bands.
  • Generally, increasing the temperature or doping
    the material will produce conduction (page
    518-519).

67
Band Theory of Metals
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