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Slide 1 of 61 General Chemistry: Chapter 12
PHILIP DUTTON
UNIVERSITY OF WINDSOR
DEPARTMENT OF CHEMISTRY AND
BIOCHEMISTRY
TENTH EDITION
GENERAL CHEMISTRY
Principles and Modern Applications
PETRUCCI HERRING MADURA BISSONNETTE
Intermolecular Forces:
Liquids and Solids 12
Copyright © 2011 Pearson Canada Inc.
Slide 2 of 61
Intermolecular Forces:
Liquids and Solids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 3 of 61
12-5 Intermolecular Forces
♦ Van der Waals Forces
•A collection of weak attractive forces between groups of
atoms or molecules.
♦ Instantaneous and Induced Dipoles
•Displacement of electrons cause polarization giving rise
to an instantaneous dipole. This dipole can affect
neighbouring molecules causing induced dipoles.
♦ Dispersion or London forces.
•Instantaneous dipole – induced dipole attraction.
•Related to polarizability.
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 4 of 61
The phenomenon of induction
♦ FIGURE 12-1
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 5 of 61
Instantaneous and induced dipoles
♦ FIGIURE 12-2
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 6 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 7 of 61
Molecular shape and polarizability
♦ FIGURE 12-3
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 8 of 61
Dipole-Dipole Interactions
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-4
♦ Dipole-dipole interactions
Slide 9 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 10 of 61
12-6 Hydrogen Bonding
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-5
♦ Comparison of boiling points of some hydrides of the elements
of groups 14, 15, 16, and 17
Slide 11 of 61
Hydrogen bonding in gaseous hydrogen fluoride
♦ FIGURE 12-6
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Electrostatic potential map of HF
Slide 12 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Hydrogen bonding between H2O molecules
Slide 13 of 61
Hydrogen bonding in water
♦ FIGURE 12-7
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
around a molecule in the solid in the liquid
Slide 14 of 61
An acetic acid dimer
♦ FIGURE 12-9
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 15 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Ethyl alcohol
(ethanol)|
at 20°C: η = 1.20 cP
Ehylene glycol
(1,2-ethanediol)|
at 20°C: η = 19.9 cP
Glycerol
(1,2,3-propanetriol)|
at 20°C: η = 1490 cP
Slide 16 of 61
Intermolecular and Intramolecular Hydrogen
Bonding
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Electrostatic potential
map of salicylic acid
showing intramolecular
hydrogen bonding.
There is no intramolecular
hydrogen bonding in
para-hydroxybenzoic acid
Hydrogen bonding between
guanine (left) and cytosine (right) in
DNA
Slide 17 of 61
12-2 Some Properties of Liquids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Cohesive Forces
Intermolecular forces between like
molecules.
Adhesive Forces
Intermolecular forces between unlike
molecules.
Surface Tension γ
Energy or work required to increase
the surface area of a liquid.
Viscosity η
A liquids resistance to flow.
FIGURE 12-10
An effect of surface tension
illustrated
Slide 18 of 61
Surface Tension
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-11
♦ Intermolecular forces in a liquid
Slide 19 of 61
Meniscus formation
♦ FIGURE 12-13
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Figure 12-14
Capillary Action
Figure 12-12
Wetting of a surface
Slide 20 of 61
Viscosity
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-15
♦ Measuring viscosity
A liquid’s resistance to flow.
The stronger the intermolecular
forces of attraction, the greater the
viscosity.
When a liquid flows, one portion of
the liquid moves with respect to
neighboring portions.
Cohesive forces within the liquid
create an internal friction, which
reduces the rate of flow.
Slide 21 of 61
increased temperature—more molecules have sufficient kinetic energy to
overcome intermolecular forces of attraction in the liquid.
increased surface area of the liquid—a greater proportion of the liquid
molecules are at the surface.
decreased strength of intermolecular forces—the kinetic energy needed
to overcome intermolecular forces of attraction is less, and more
molecules have enough energy to escape.
Enthalpy of Vaporization
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
ΔHvap = Hvapor – Hliquid = - ΔHcondensation
Slide 22 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 23 of 61
Vapor Pressure of Liquids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-16
♦ Establishing liquid-vapor equilibrium
liquid vapor
vaporization
condensation
Slide 24 of 61
Vapor pressure illustrated
♦ FIGURE 12-17
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Mercury
manometer
Vapor
pressure
of liquid
Pvap
independent
of Vliq
Pvap
independent
of Vgas
Pvap
dependent on
T
Slide 25 of 61
Vapor pressure curves of several liquids
♦ FIGURE 12-18
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 26 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 27 of 61
An Equation for Expressing Vapor
Pressure Data
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-20
♦ Vapor pressure data plotted as lnP versus 1/T
ln P = -A ( ) + B
1
T
A =
ΔHvap
R
ln = - ( - )
P2
P1
1
T2
1
T1
ΔHvap
R
Slide 28 of 61
Boiling and Boiling Point
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-21
♦ Boiling water in a paper cup
Liquid boils at low
pressure
FIGURE12-21
Boiling water in a paper cup
Slide 29 of 61
The Critical Point
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-22
♦ Attainment of the critical point for benzene
Slide 30 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 31 of 61
12-3 Some Properties of Solids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Figure 12-23
Cooling curve for water
Figure 12-24
Heating curve for water
Melting, Melting Point, and Heat of Fusion
H2O(s) H2O(l) ΔHfus(H2O) = +6.01 kJ/mol
Slide 32 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 33 of 61
Sublimation
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-25
♦ Sublimation of iodine
ΔHsub = ΔHfus + ΔHvap
= -ΔHdeposition
Slide 34 of 61
12-4 Phase Diagrams
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-26
♦ Temperature, pressure, and states of matter
Slide 35 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-27
♦ Phase diagram for iodine
Iodine
Slide 36 of 61
Carbon Dioxide
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-28
♦ Phase diagram for carbon dioxide
Slide 37 of 61
Supercritical Fluids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-29
♦ Critical point and critical isotherm
Slide 38 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Decaffeinated
coffee
Slide 39 of 61
Water
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-30
♦ Phase diagram for water
Slide 40 of 61
Phases and Phase Transitions
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
melting (s) (l)
vaporization (l) (g)
sublimation (s) (g)
freezing (l) (s)
condensation (g) (l)
deposition (g) (s)
Slide 41 of 61
12-7 Network Covalent Solids and
Ionic Solids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-32
♦ The diamond structure
Figure 12-33
The graphite structure
Slide 42 of 61
Other Allotropes of Carbon
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-34
♦ Fullerenes
Slide 43 of 61
Nanotubes
♦ FIGURE 12-35
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 44 of 61
Ionic Solids
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-36
♦ Interionic forces of attraction
Slide 45 of 61
12-8 Crystal Structures
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-37
♦ The cubic lattice
Slide 46 of 61
Unit cells in the cubic crystal system
♦ FIGURE 12-38
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 47 of 61
Closest packed structures
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦A closest packed pyramid of cannonballs. Oranges at a fruit stand are often
packed in cubic closest packed pyramids so that they will not slip.
Slide 48 of 61
Closest packed structures
♦ FIGURE 12-39
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 49 of 61
A face-centered cubic unit cell for the cubic closest packing of
spheres
♦ FIGURE 12-40
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 50 of 61
The hexagonal closest packed (hcp) crystal structure
♦ FIGURE 12-41
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 51 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Illustrating the coordination number for the hcp and ccp structures
Slide 52 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
How spheres are shared between or among unit cells
Slide 53 of 61
Apportioning atoms among cubic unit cells
♦ FIGURE 12-42
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 54 of 61
X-Ray Diffraction
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-43
♦ Diffraction of X-rays by a crystal
Slide 55 of 61
Determination of crystal structure by X-ray diffraction
♦ FIGURE 12-44
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 56 of 61
Ionic Crystal Structures
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-46
♦ Holes in face-centered cubic unit cell
Figure 12-47
Cross section of an octahedral hole
Slide 57 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 58 of 61
Some units of greater complexity
♦ FIGURE 12-50
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 59 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
Slide 60 of 61
12-7 Energy Changes in the Formation of Ionic
Crystals
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
♦ FIGURE 12-51
♦ Enthalpy diagram for the formation of an ionic crystal
Slide 61 of 61
End of Chapter Questions
♦You can think about problems in reverse to
help sort out a strategy.
Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
If I had the
answer, what
would I have
used to get it.
a
b
c Solution
Found

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Introduction to-chemistry

  • 1. Slide 1 of 61 General Chemistry: Chapter 12 PHILIP DUTTON UNIVERSITY OF WINDSOR DEPARTMENT OF CHEMISTRY AND BIOCHEMISTRY TENTH EDITION GENERAL CHEMISTRY Principles and Modern Applications PETRUCCI HERRING MADURA BISSONNETTE Intermolecular Forces: Liquids and Solids 12 Copyright © 2011 Pearson Canada Inc.
  • 2. Slide 2 of 61 Intermolecular Forces: Liquids and Solids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 3. Slide 3 of 61 12-5 Intermolecular Forces ♦ Van der Waals Forces •A collection of weak attractive forces between groups of atoms or molecules. ♦ Instantaneous and Induced Dipoles •Displacement of electrons cause polarization giving rise to an instantaneous dipole. This dipole can affect neighbouring molecules causing induced dipoles. ♦ Dispersion or London forces. •Instantaneous dipole – induced dipole attraction. •Related to polarizability. Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 4. Slide 4 of 61 The phenomenon of induction ♦ FIGURE 12-1 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 5. Slide 5 of 61 Instantaneous and induced dipoles ♦ FIGIURE 12-2 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 6. Slide 6 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 7. Slide 7 of 61 Molecular shape and polarizability ♦ FIGURE 12-3 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 8. Slide 8 of 61 Dipole-Dipole Interactions Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-4 ♦ Dipole-dipole interactions
  • 9. Slide 9 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 10. Slide 10 of 61 12-6 Hydrogen Bonding Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-5 ♦ Comparison of boiling points of some hydrides of the elements of groups 14, 15, 16, and 17
  • 11. Slide 11 of 61 Hydrogen bonding in gaseous hydrogen fluoride ♦ FIGURE 12-6 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Electrostatic potential map of HF
  • 12. Slide 12 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Hydrogen bonding between H2O molecules
  • 13. Slide 13 of 61 Hydrogen bonding in water ♦ FIGURE 12-7 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 around a molecule in the solid in the liquid
  • 14. Slide 14 of 61 An acetic acid dimer ♦ FIGURE 12-9 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 15. Slide 15 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Ethyl alcohol (ethanol)| at 20°C: η = 1.20 cP Ehylene glycol (1,2-ethanediol)| at 20°C: η = 19.9 cP Glycerol (1,2,3-propanetriol)| at 20°C: η = 1490 cP
  • 16. Slide 16 of 61 Intermolecular and Intramolecular Hydrogen Bonding Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Electrostatic potential map of salicylic acid showing intramolecular hydrogen bonding. There is no intramolecular hydrogen bonding in para-hydroxybenzoic acid Hydrogen bonding between guanine (left) and cytosine (right) in DNA
  • 17. Slide 17 of 61 12-2 Some Properties of Liquids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Cohesive Forces Intermolecular forces between like molecules. Adhesive Forces Intermolecular forces between unlike molecules. Surface Tension γ Energy or work required to increase the surface area of a liquid. Viscosity η A liquids resistance to flow. FIGURE 12-10 An effect of surface tension illustrated
  • 18. Slide 18 of 61 Surface Tension Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-11 ♦ Intermolecular forces in a liquid
  • 19. Slide 19 of 61 Meniscus formation ♦ FIGURE 12-13 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Figure 12-14 Capillary Action Figure 12-12 Wetting of a surface
  • 20. Slide 20 of 61 Viscosity Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-15 ♦ Measuring viscosity A liquid’s resistance to flow. The stronger the intermolecular forces of attraction, the greater the viscosity. When a liquid flows, one portion of the liquid moves with respect to neighboring portions. Cohesive forces within the liquid create an internal friction, which reduces the rate of flow.
  • 21. Slide 21 of 61 increased temperature—more molecules have sufficient kinetic energy to overcome intermolecular forces of attraction in the liquid. increased surface area of the liquid—a greater proportion of the liquid molecules are at the surface. decreased strength of intermolecular forces—the kinetic energy needed to overcome intermolecular forces of attraction is less, and more molecules have enough energy to escape. Enthalpy of Vaporization Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ΔHvap = Hvapor – Hliquid = - ΔHcondensation
  • 22. Slide 22 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 23. Slide 23 of 61 Vapor Pressure of Liquids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-16 ♦ Establishing liquid-vapor equilibrium liquid vapor vaporization condensation
  • 24. Slide 24 of 61 Vapor pressure illustrated ♦ FIGURE 12-17 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Mercury manometer Vapor pressure of liquid Pvap independent of Vliq Pvap independent of Vgas Pvap dependent on T
  • 25. Slide 25 of 61 Vapor pressure curves of several liquids ♦ FIGURE 12-18 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 26. Slide 26 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 27. Slide 27 of 61 An Equation for Expressing Vapor Pressure Data Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-20 ♦ Vapor pressure data plotted as lnP versus 1/T ln P = -A ( ) + B 1 T A = ΔHvap R ln = - ( - ) P2 P1 1 T2 1 T1 ΔHvap R
  • 28. Slide 28 of 61 Boiling and Boiling Point Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-21 ♦ Boiling water in a paper cup Liquid boils at low pressure FIGURE12-21 Boiling water in a paper cup
  • 29. Slide 29 of 61 The Critical Point Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-22 ♦ Attainment of the critical point for benzene
  • 30. Slide 30 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 31. Slide 31 of 61 12-3 Some Properties of Solids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Figure 12-23 Cooling curve for water Figure 12-24 Heating curve for water Melting, Melting Point, and Heat of Fusion H2O(s) H2O(l) ΔHfus(H2O) = +6.01 kJ/mol
  • 32. Slide 32 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 33. Slide 33 of 61 Sublimation Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-25 ♦ Sublimation of iodine ΔHsub = ΔHfus + ΔHvap = -ΔHdeposition
  • 34. Slide 34 of 61 12-4 Phase Diagrams Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-26 ♦ Temperature, pressure, and states of matter
  • 35. Slide 35 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-27 ♦ Phase diagram for iodine Iodine
  • 36. Slide 36 of 61 Carbon Dioxide Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-28 ♦ Phase diagram for carbon dioxide
  • 37. Slide 37 of 61 Supercritical Fluids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-29 ♦ Critical point and critical isotherm
  • 38. Slide 38 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Decaffeinated coffee
  • 39. Slide 39 of 61 Water Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-30 ♦ Phase diagram for water
  • 40. Slide 40 of 61 Phases and Phase Transitions Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 melting (s) (l) vaporization (l) (g) sublimation (s) (g) freezing (l) (s) condensation (g) (l) deposition (g) (s)
  • 41. Slide 41 of 61 12-7 Network Covalent Solids and Ionic Solids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-32 ♦ The diamond structure Figure 12-33 The graphite structure
  • 42. Slide 42 of 61 Other Allotropes of Carbon Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-34 ♦ Fullerenes
  • 43. Slide 43 of 61 Nanotubes ♦ FIGURE 12-35 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 44. Slide 44 of 61 Ionic Solids Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-36 ♦ Interionic forces of attraction
  • 45. Slide 45 of 61 12-8 Crystal Structures Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-37 ♦ The cubic lattice
  • 46. Slide 46 of 61 Unit cells in the cubic crystal system ♦ FIGURE 12-38 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 47. Slide 47 of 61 Closest packed structures Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦A closest packed pyramid of cannonballs. Oranges at a fruit stand are often packed in cubic closest packed pyramids so that they will not slip.
  • 48. Slide 48 of 61 Closest packed structures ♦ FIGURE 12-39 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 49. Slide 49 of 61 A face-centered cubic unit cell for the cubic closest packing of spheres ♦ FIGURE 12-40 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 50. Slide 50 of 61 The hexagonal closest packed (hcp) crystal structure ♦ FIGURE 12-41 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 51. Slide 51 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 Illustrating the coordination number for the hcp and ccp structures
  • 52. Slide 52 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 How spheres are shared between or among unit cells
  • 53. Slide 53 of 61 Apportioning atoms among cubic unit cells ♦ FIGURE 12-42 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 54. Slide 54 of 61 X-Ray Diffraction Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-43 ♦ Diffraction of X-rays by a crystal
  • 55. Slide 55 of 61 Determination of crystal structure by X-ray diffraction ♦ FIGURE 12-44 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 56. Slide 56 of 61 Ionic Crystal Structures Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-46 ♦ Holes in face-centered cubic unit cell Figure 12-47 Cross section of an octahedral hole
  • 57. Slide 57 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 58. Slide 58 of 61 Some units of greater complexity ♦ FIGURE 12-50 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 59. Slide 59 of 61 Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12
  • 60. Slide 60 of 61 12-7 Energy Changes in the Formation of Ionic Crystals Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 ♦ FIGURE 12-51 ♦ Enthalpy diagram for the formation of an ionic crystal
  • 61. Slide 61 of 61 End of Chapter Questions ♦You can think about problems in reverse to help sort out a strategy. Copyright © 2011 Pearson Canada Inc.General Chemistry: Chapter 12 If I had the answer, what would I have used to get it. a b c Solution Found

Editor's Notes

  1. In this chapter, you will learn how to deduce and write chemical formulas and how to use the information incorporated into chemical formulas. The chapter ends with an overview of the relationship between names and formulas—chemical nomenclature.
  2. A scanning tunneling microscope image of 48 iron atoms adsorbed onto a surface of copper atoms. The iron atoms were moved into position with the tip of the scanning tunneling microscope in order to create a barrier that forced some electrons of the copper atoms into a quantum state seen here as circular rings of electron density. The colors are from the computer rendering of the image. In this chapter we discuss the periodic table and the properties of atoms and ions. In this chapter, we will use the table as a backdrop for a discussion of some properties of elements, including atomic radii, ionization energies, and electron affinities. These atomic properties also arise in the discussion of chemical bonding in the following two chapters, and the periodic table itself will be our indispensable guide throughout much of the remainder of the text.
  3. The attraction of a balloon to a surface is a commonplace example of induction. The balloon is charged by rubbing, and the charged balloon induces an opposite charge on the surface. (See also Appendix B.)
  4. In the normal condition, a nonpolar molecule has a symmetrical charge distribution. In the instantaneous condition, a displacement of the electronic charge produces an instantaneous dipole with a charge separation represented as δ+ and δ- . In an induced dipole, the instantaneous dipole on the left induces a charge separation in the molecule on the right. The result is an instantaneous dipole–induced dipole attraction.
  5. ≤10 kJ /mol
  6. 5-20 kJ /mol
  7. 15 to 40 kJ/mol The boiling points for NH3, H2O and HF are unusually high compared with those of other members of their groups.
  8. In gaseous hydrogen fluoride, many of the HF molecules are associated into cyclic (HF6) structures of the type pictured here. Each H atom is bonded to one F atom by a single covalent bond (-) and to another F atom through a hydrogen bond (…).
  9. Each water molecule is linked to four others through hydrogen bonds. The arrangement is tetrahedral. Each H atom is situated along a line joining two O atoms, but closer to one O atom (100 pm) than to the other (180 pm). For the crystal structure of ice, H atoms lie between pairs of O atoms, again closer to one O atom than to the other. (Molecules behind the plane of the page are light blue.) O atoms are arranged in bent hexagonal rings arranged in layers. This characteristic pattern is similar to the hexagonal shapes of snowflakes. In the liquid, water molecules have hydrogen bonds to only some of their neighbours. This allows the water molecules to pack more densely in the liquid than in the solid.
  10. Despite being denser than water, the needle is supported on the surface of the water. The property of surface tension accounts for this unexpected behaviour.
  11. Molecules at the surface are attracted only by other surface molecules and by molecules below the surface. Molecules in the interior experience forces from neighbouring molecules in all directions.
  12. Wetting of a surface Water spreads into a thin film on a clean glass surface (left). If the glass is coated with oil or grease, the adhesive forces between the water and oil are not strong enough to spread the water, and droplets stand on the surface (right). Meniscus formation Water wets glass (left). The meniscus is concave—the bottom of the meniscus is below the level of the water–glass contact line. Mercury does not wet glass. The meniscus is convex—the top of the meniscus is above the mercury–glass contact line. Capillary action A thin film of water spreads up the inside walls of the capillary because of strong adhesive forces between water and glass (water wets glass). The pressure below the meniscus falls slightly. Atmospheric pressure then pushes a column of water up the tube to eliminate the pressure difference. The smaller the diameter of the capillary, the higher the liquid rises. Because its magnitude is also directly proportional to surface tension, capillary rise provides a simple experimental method of determining surface tension, described in Exercise 119.
  13. By measuring the velocity of a ball dropping through a liquid, a measure of the liquid viscosity can be obtained.
  14. A liquid is allowed to evaporate into a closed container. Initially, only vaporization occurs. Condensation begins. The rate at which molecules evaporate is greater than the rate at which they condense, and the number of molecules in the vapor state continues to increase. The rate of condensation is equal to the rate of vaporization. The number of vapor molecules remains constant over time, as does the pressure exerted by this vapor.
  15. A mercury barometer. The pressure exerted by the vapor in equilibrium with a liquid injected to the top of the mercury column depresses the mercury level. Compared with (b), the vapor pressure is independent of the volume of liquid injected. Compared with (c), the vapor pressure is independent of the volume of vapor present. Vapor pressure increases with an increase in temperature.
  16. An empty paper cup heated over a Bunsen burner quickly bursts into flame. If a paper cup is filled with water, it can be heated for an extended time as the water boils. This is possible for three reasons: Because of the high heat capacity of water, heat from the burner goes primarily into heating the water, not the cup. As the water boils, large quantities of heat (ΔHvap) are required to convert the liquid to its vapor. The temperature of the cup does not rise above the boiling point of water as long as liquid water remains. The boiling point of 99.9 °C instead of 100°C suggests that the prevailing barometric pressure was slightly below 1 atm.
  17. In a sealed container, the meniscus separating a liquid from its vapor is just barely visible at the instant the critical point is reached. At the critical point—the liquid and vapor become indistinguishable.
  18. Even at temperatures well below its melting point of 114°C, solid iodine exhibits an appreciable sublimation pressure. Here, purple iodine vapor is produced at about 70°C. Deposition of the vapor to solid iodine occurs on the colder walls of the flask.
  19. The outline of a phase diagram is suggested by the distribution of points. red points identify the temperatures and pressures at which solid is the stable phase blue points identify the temperatures and pressures at which liquid is the stable phase brown points represent the temperatures and pressures at which gas is the stable phase. (Details follow for specific cases on next slides)
  20. Applying pressure to a gas at temperatures below the critical isotherm, Tc, causes a liquid to form with the appearance of a meniscus, a discontinuous phase change. Applying pressure above the critical isotherm simply increases the density of the supercritical fluid. In a path traced by the small arrows, gas changes to liquid without exhibiting a discontinuous phase transition.
  21. “Naturally” decaffeinated coffee is made through a process that uses supercritical fluid CO2 as a solvent to dissolve the caffeine in green coffee beans. Afterward, the beans are roasted and sold to consumers.
  22. Point O, the triple point, is at 0.0098°C and 4.58 mmHg. (The normal melting point is at exactly 0°C and 760 mmHg.) The critical point, C, is at 374.1°C and 218.2 atm. At point D the temperature is -22.0°C and the pressure is 2045 atm. The negative slope of the fusion curve, OD (greatly exaggerated here), and the significance of the broken straight lines are discussed in the text.
  23. An icosahedron, a shape formed by 20 equilateral triangles. Five triangles meet at each of the 12 vertices. Truncating or cutting off a vertex reveals a new pentagonal face. The truncated icosahedron. Twelve pentagons have replaced the original 12 vertices, and the 20 equilateral triangles have been replaced by 20 hexagons. The C60 molecule.
  24. Ball-and-stick model of a small nanotube. A bundle of single-wall nanotubes.
  25. Because of the higher charges on the ions and the closer proximity of their centers, the interionic attractive force between Mg2+ and Cl- is about seven times as great as between Na+ and Cl-.
  26. One parallelepiped formed by the intersection of mutually perpendicular planes is shaded in green—it is a cube. An endless lattice can be generated by simple displacements of the green cube in the three perpendicular directions (that is, left and right, up and down, and forward and backward).
  27. Spheres in layer A are red. Those in layer B are yellow, and in layer C, blue. The holes in closest packed structures. The trigonal hole is formed by three spheres in one of the layers. The tetrahedral hole is formed when a sphere in the upper layer sits in the dimple of the lower layer. The octahedral hole is formed between two groups of three spheres in two layers.
  28. The 14 spheres on the left are extracted from a larger array of spheres in a cubic closest packed structure. The two middle layers each have six atoms; the top and bottom layers, one. Rotation of the group of 14 spheres reveals the fcc unit cell (right).
  29. A unit cell is highlighted in heavy green lines. The atoms that are part of that cell are joined in solid lines. Note that the unit cell is a parallelepiped but not a cube. Three adjoining unit cells are depicted. The highlighted unit cell and broken-line regions together show the layering (ABA) described in Figure 12-39. The hexagonal prism showing parts of the shared spheres at the corners and the single sphere at the center of the unit cell.
  30. For a sphere in the middle of the unit cell, there is no sharing; on a face 1 2 of the sphere is in the unit cell; at an edge only 1 4 of the sphere is in the unit cell; and in a corner only 1 8 is contained within the unit cell.
  31. In X-ray diffraction, the scattering is usually from no more than 20 planes deep in a crystal. The size of the single crystal is to have enough of the surface available for diffraction, yet the diffraction is dominated by a few of the surface planes.
  32. The two triangles outlined by dashed lines are identical. The hypotenuse of each triangle is equal to the interatomic distance, d. The side opposite the angle thus has a length of d sin u. Wave b travels farther than wave a by the distance 2d sin u.
  33. For clarity, only the centers of the ions are shown. Oppositely charged ions are actually in contact. We can think of this structure as an fcc lattice of Cl- ions, with Na+ ions filling the octahedral holes. The Cs+ ion is in the center of the cube, with Cl- ions at the corners. In reality, each Cl- is in contact with the ion. An alternative unit cell has Cl- at the center and Cs+ at the corners.
  34. Shown here is a five-step sequence for the formation of one mole of NaCl(s) from its elements in their standard states. The sum of the five enthalpy changes gives ΔH°f[NaCl(s)]. The equivalent one-step reaction for the formation of NaCl(s) directly from Na(s) and Cl2(g) is shown in color. (The vertical arrows representing ΔH values are not to scale.)