“Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin...

93
“Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1

Transcript of “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin...

Page 1: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

“Do me a solid..”the story of the other 2 states of

matter

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

1

Page 2: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

2

Gas, The oddball of the trio:The Three States of Matter

compared

Page 3: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Solids/Liquids compared to gas

• H2O (s) H2O(l) Δ H = 6 kJ/mol

• H2O (l) H2O(g) Δ H = 41 kJ/mol

• s/l slightly compressible, density similar (see table 10.1)

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

3

Page 4: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

4

Intermolecular Forces

Forces between (not within) molecules in

“condensed states”

dipole-dipole attraction: molecules with dipoles orient themselves so that “+” and “” ends attract

hydrogen bonds: dipole-dipole attraction in which hydrogen is bound to a highly electronegative atom. (F, O, N)

Page 5: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Figure 10.2Dipole-Dipole Attractions 1% as strong as

the covalent/ionic

bond.

Rapidly weaken with

increase distance

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

5

Page 6: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Figure 10.3 A Water Molecule

H-bonding strong:

small H

big electro. Diff

Water: high melting/

boiling points – to

overcome this force

Also seen with H-F,

H-N bonds

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

6

Page 7: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

7

Figure 10.4The Boiling Points of the Covalent Hydrides of the

Elements in Groups 4A, 5A, 6A, and 7AH-bonding for H-O, H-F, H-N

Page 8: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

8

What about non-polar molecules and noble gases when condensed? :

London Dispersion Forces

Page 9: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

9

London Dispersion Forces

relatively weak forces that exist among noble gas atoms and nonpolar molecules when in the condensed state (Ar, C8H18)

caused by instantaneous dipole, in which electron distribution becomes asymmetrical.

Page 10: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

London Forces

• the ease with which electron “cloud” of an atom can be distorted is called polarizability.

• Large molecules, more polarizable.

Explain Table 10.2, pg. 455.

Explain the trend in Halogen b.p.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

10

Page 11: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

11

Focus on Liquid Properties

Surface Tension

Capillary Action

Viscosity

Page 12: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Surface Tension: The resistance to an increase in its surface area (polar

molecules).

Page 13: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Surface tension explained

Page 14: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Capillary Action: Spontaneous rising of a liquid in a narrow tube.

• Cohesion vs. Adhesion

Page 15: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Viscosity: Resistance to flow (molecules with large intermolecular

forces).

15

• High IF, high viscosity (thickness) Ex. Glycerol, gasoline vs. grease

• Ex: add xanthan gum to water, increases the viscosity

Page 16: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

16

Focus on Solids: Types of Solids

Crystalline Solids: highly regular arrangement of their components [table salt (NaCl), pyrite (FeS2)].

Amorphous solids: considerable disorder in their structures (glass).

Page 17: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

17

Crystalline Solid

Lattice: A 3-dimensional system of points designating the centers of components (atoms, ions, or molecules) that make up the substance.

Unit Cell: The smallest repeating unit of the lattice. simple cubic

Page 18: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Unit CellsUnit Cells

Page 19: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Unit CellsUnit Cells• Three common types of unit cell.

– Simple cubic, atoms at the corners of a simple cube,• each atom shared by 8 unit cells;

– Body-centered cubic (bcc), atoms at the corners of a cube plus one in the center of the body of the cube,

• corner atoms shared by 8 unit cells, center atom completely enclosed in one unit cell;

– Face-centered cubic (fcc), atoms at the corners of a cube plus one atom in the center of each face of the cube,

– corner atoms shared by 8 unit cells, face atoms shared by 2 unit cells.

Unit CellsUnit Cells• Three common types of unit cell.

– Simple cubic, atoms at the corners of a simple cube,• each atom shared by 8 unit cells;

– Body-centered cubic (bcc), atoms at the corners of a cube plus one in the center of the body of the cube,

• corner atoms shared by 8 unit cells, center atom completely enclosed in one unit cell;

– Face-centered cubic (fcc), atoms at the corners of a cube plus one atom in the center of each face of the cube,

– corner atoms shared by 8 unit cells, face atoms shared by 2 unit cells.

Page 20: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

20

Figure 10.9Three Cubic Unit Cells and the Corresponding Lattices

Page 21: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Crystal Structure of Sodium ChlorideCrystal Structure of Sodium Chloride• Face-centered cubic.• Two equivalent ways of defining unit

cell:– Cl- (larger) ions at the corners of the cell, or– Na+ (smaller) ions at the corners of the cell.

• The cation :anion ratio in the unit cell must be a 1:1, since formula is NaCl

• Visualize face center Cl-, Na+ in spaces

Page 22: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Crystal Structure of Sodium ChlorideCrystal Structure of Sodium Chloride

Page 23: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

How many Na+, Cl- do you see? Count them!

Page 24: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Body Center = 1 unit

Face Center = 1/2 unit

Edge = 1/4 unit

Corner = 1/8 unit

Page 25: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Three Cubic Unit Cells

and the Correspondin

g Lattices

Page 26: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

26

How do we determine crystal structure? Interference of x-rays can show us the distance between the particles in the

crystal

Page 27: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

the Bragg Equation

• sin θ = xy/d, so xy=d sin θ and yz =d sin θ

• So, xy + yz = d sin θ + d sin θ = 2d sin θ

• For in phase xy + yz = nλ27

Page 28: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

The Bragg Equation

• xy + yz = nλ

• xy + yz = 2d sin θ ,

• So, n = 2d sin • d = distance between atoms

n = an integer

= wavelength of the x-rays

See problems 10.1, pg 461 28

Page 29: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

29

Bragg Equation

Used for analysis of crystal structures.

n = 2d sin

d = distance between atoms

n = an integer

= wavelength of the x-rays

Page 30: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

30

Types of Crystalline SolidsIonic Solid: contains ions at the points of the lattice that describe the structure of the solid (NaCl).

Molecular Solid: discrete covalently bonded molecules at each of its lattice points (sucrose, ice).

Atomic Solid: atoms at the lattice points. Three kinds of atomic solids: network, metals, group 18. (ex: diamond, Cu, Ar)

Page 31: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

31

Figure 10.12 Examples of Three Types of Crystalline Solids

Page 32: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Atomic solids compared

• Network, diamond, covalent mp= 3500 C

• Metallic, Cu, delocalized cov., mp = 1083 C

• Group 18, Ar, London, mp = -189 C

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

32

Page 33: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

33

Packing in Metals

• Model: closest packing

• atoms/molecules/ions as spheres.

• To maximize IF forces: sphere packed as

close as possible.

• Small spaces exist between adjacent spheres: called interstitial holes.

Page 34: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Two types of packing possible

hexagonal closest packed (“hcp”)

resulting from aba

cubic closest packed (“ccp”)

resulting from abca

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

34

Page 35: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Let’s pack a crystal hcp and ccpLet’s pack a crystal hcp and ccp 1. Form a base layer of 3 sphere. 2. Place 2nd layer to occupy dimples in layer 1. (one choice only) 3. Two choices for the third layer of

spheres:– 3rd layer over 1st layer(ABAB). Hexagonal

close packing (hcp);– 3rd layer is not over 1st layer. 4th layer is

over 1st layer . (ABCABC. Cubic close packing (ccp).

Page 36: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.
Page 37: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Choose: which one is ccp, which one is hcp?

Close Packing of SpheresClose Packing of Spheres

Page 38: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

38

Figure 10.14Hexagonal Closest Packing

Page 39: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

39

Figure 10.15Cubic Closest Packing

Page 40: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Structures of SolidsStructures of Solids

Close Packing of SpheresClose Packing of Spheres• Each sphere is surrounded by 12 other

spheres (6 in one plane, 3 above and 3 below).

• Coordination number: the number of spheres directly surrounding a central sphere.

• If unequally sized spheres are used, the smaller spheres are placed in the interstitial holes.

Page 41: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

The Indicated Sphere Has 12

Nearest Neighbors

True for bothccp and hcp

Page 42: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

42

Figure 10.15 Cubic Closest Packing

Page 43: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

43

Figure 10.16The Indicated Sphere Has 12 Nearest Neighbors

Page 44: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Compay. All rights reserved.

44

Bonding Models for Metals

We can explain why metals are malleable, ductile and conduct heat/electricity

Electron Sea Model: A regular array of metal cations awash in a “sea” of electrons. Band (Molecular Orbital) Model: Electrons assumed to travel around metal crystal in MOs formed from valence atomic orbitals of metal atoms.

Page 45: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

45

Figure 10.18The Electron Sea Model for Metals Postulates

a Regular Array of Cations in a “Sea” of Valence Electrons

Page 46: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Figure 10.19The Molecular Orbital Energy Levels Produced When Various Numbers of Atomic Orbitals Interact.

• 2 ao’s make 2MOs• When 4 ao’s overlap,

4MOs

• Note: when many MO are available, “bands” become virtually

continuous.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

46

Page 47: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

The Band Model for Magnesium

• Core electrons are localized, but valence are in closely spaced Mos: conduction bands.

• Electrons move into empty MOs

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

47

Page 48: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

48

Figure 10.21Two Types of Alloys

Page 49: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

49

Metal Alloys

1. Substitutional Alloy: some metal atoms replaced by others of similar size.

brass = Cu/Zn

Sterling silver: Ag/Cu

Pewter: tin/Cu/Bi/Sb

Substances that have a mixture of elements and Substances that have a mixture of elements and metallic properties.metallic properties.

Page 50: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

50

Metal Alloys(continued)

2. Interstitial Alloy: Interstices (holes) in closest packed metal structure are

occupied by small atoms. Ex:

--steel = iron, carbon in the holes

--increase C, reduce ductility, increase hardness and strength.

Mild steel: 0.2% C, nails, chains

Medium: 0.2-0.6% C: beams

High: 1.5% C: springs, tools, knives

Page 51: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Metal alloys

• Alloy steel: mix of interstitial , C and substitutional.

• Ex: stainless steel Fe, C and 11% Cr.

• Cr forms layer of Cr oxide, prevent rust.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

51

Page 52: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

52

Network Solids

Composed of strong directional covalent bonds that are best viewed as a “giant molecule”.

brittle may or may not conduct heat or electricity carbon, silicon-based

graphite, diamond, ceramics, glass

Page 53: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

53

Figure 10.22The Structures of Diamond and Graphite: both network solids

Page 54: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Why is diamond insulator not conductor?

a)Carbon in diamond Empty MOs much higher E

b)Metal: Empty MOs close in E

54

Page 55: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

55

However, Graphite is a conductor:--each C is sp2, not sp3 like diam.--The p Orbitals in graphite form pi bonds: increase stab. layers & allow conductivity -

Page 56: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Layers in graphite

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

56

Page 57: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Graphite vs. Diamod

• Graphite: conducts, soft, strong bonding in layers, weak between. Layers slide past:

good for lubricant, pencils.

Density: 2.2 g/cc

• Diamond: does not conducts, hardest, strong bonding all around. Good for cutting

Density: 3.5 g/cc

Copyright©2000 by Houghton

Mifflin Company. All rights reserved.

57

Page 58: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Si: the carbon of geology

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

58

Page 59: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Si, right under C but different

• No long Si-Si chains like C

• Si forms chains of Si-O

• SiO2 = e.f. of silica, most important

• Not CO2 structure, Si cannot

overlap p’s w/ O. No pi bonds.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

59

Page 60: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

• How does Si bond with O?

• A network of SiO4 tetrahedrons.

• No indiv. SiO2, although this is e.f.

• This is quartz

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

60

Page 61: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

61

Glass: melt quartz, cool rapidly: (a) a Quartz Crystal (b) a Quartz Glass

Additives: see table 10.5 Ex: add B2O3 to make borosilcate glass

Page 62: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

62

Silicate Anions: Note all are based on SiO4 tetrahedron

Page 63: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Ceramics

• Made from clays (contain silicates) that are hardened by firing at high T.

• Non-metallic: silicates bind with cations as clay is dried, trapping crystals of kaolinite.

• Strong, brittle, heat/chemical resistant

63

Page 64: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Semiconductors

• Si: Like C, large gap to empty MOs but Si: Like C, large gap to empty MOs but gap is smaller, so some electrons can cross gap is smaller, so some electrons can cross the band gap.the band gap.

• Si is a semiconductor.Si is a semiconductor.

• Conductivity is enhanced by doping with group 13 or group 15 elements.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

64

Page 65: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Silicon Crystal Doped with (a) Arsenic and (b) Boron

• As: 1 extra valence e-

n-type semiconductor

extra e- can join the conduction band

B: l less valence e-:

p-type semiconductor

creates a “hole” that is filled by an e- from Si.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

65

Page 66: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

66

Figure 10.30Energy Level Diagrams for (a) an n-Type

Semiconductor and (b) a p-Type Semiconductor

Page 67: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

The p-n Junction • e- flow from n to p to

fill “holes”

p side becomes neg• (b) battery with – at

n and + at p. e- flow back: reverse bias, current does not flow

(c) battery other way e- flow right way: forward bias

Application:Transistors:

switches : chips: iphone

67

Page 68: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Molecular Solids

• Ice

• Dry ice: CO2

• S8

• P4

What forces between molecules in above crystals?

Why is S8 solid?Copyright©2000 by Houghton

Mifflin Company. All rights reserved.

68

Page 69: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Ionic Solids

• High melting pt• Larger Ions (anions) in

hcp or ccp structure Cations fit in the holes

3 types of holes.

trig< tetra<octa• trig never occupied

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

69

Page 70: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

70

Figure 10.33The Holes that Exist Among Closest Packed Uniform Spheres

Page 71: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

71

Tetrahedral Holes in a Face-Centered Cubic Unit Cell Ex. ZnS S2- face centered. Zn2+ in tetrahedral holes Q: How many tetrahedral holes? How many are occupied?

Page 72: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

NaCl revisited

• Cl- face-centered from ccp packing

• Na+ in all octahedral holes.

• Q: how many octa

holes in (a).

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

72

Page 73: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

NaCl octahedral holes

• Note: center Na+

surrounded by the

6 face-centered Cl-

73

Page 74: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

74

Vapor Pressure

. . . is the pressure of the vapor present at equilibrium.

. . . is determined principally by the size of the intermolecular forces in the liquid.

. . . increases significantly with temperature.

Volatile liquids have high vapor pressures.

Page 75: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

75

Figure 10.36Behavior of a Liquid in a Closed Container

Page 76: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

76

Figure 10.37The Rates of Condensation and

Evaporation

Page 77: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

77

Figure 10.38Vapor Pressure

Page 78: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

78

Figure 10.39The Number of Molecules in a Liquid With a Given Energy Versus Kinetic

Energy at Two Temperatures

Page 79: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

79

Figure 10.40The Vapor Pressure of Water

Page 80: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

80

Figure 10.42 Heating Curve for Water

Page 81: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

81

Melting Point

Molecules break loose from lattice points and solid changes to liquid. (Temperature is constant as melting occurs.)

vapor pressure of solid = vapor pressure of liquid

Page 82: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

82

Figure 10.43The Vapor Pressures of Solid and Liquid Water

Page 83: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

83

Figure 10.44An Apparatus that Allows Solid and Liquid Water to Interact Only Through the Vapor State

Page 84: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

84

Figure 10.45Water in a Closed System

Page 85: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

85

Figure 10.46The Supercooling of Water

Page 86: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

86

Boiling Point

Constant temperature when added energy is used to vaporize the liquid.

vapor pressure of liquid = pressure of surrounding atmosphere

Page 87: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

87

Phase Diagram

Represents phases as a function of temperature and pressure.

critical temperature: temperature above which the vapor can not be liquefied.

critical pressure: pressure required to liquefy AT the critical temperature.

critical point: critical temperature and pressure (for water, Tc = 374°C and 218 atm).

Page 88: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

88

Figure 10.47The Phase Diagram for Water

Page 89: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

89

Figure 10.48Diagrams of Various Heating Experiments

Page 90: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

90

Figure 10.49The Phase Diagram for Water

Page 91: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

91

Figure 10.52The Phase Diagram for Carbon Dioxide

Page 92: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

92

Figure 10.50 A Schematic of Two Circuits Connected by a Transistor

Page 93: “Do me a solid..” the story of the other 2 states of matter Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1.

Copyright©2000 by Houghton Mifflin Company. All rights

reserved.

93

Figure 10.51The Steps for Forming a Transistor in a Crystal of Initially

Pure Silicon