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1

Chapter 10

Liquids, Solids, and Phase Changes

2

Gases, Liquids and Solids

•Gases have little or no interactions.

•Liquids and solids have significant interactions.

3

Gases, Liquids and Solids

•Liquids and solids have well-defined volume.

•Liquid molecules “flow,” while solids are held “rigid.”

4

Intermolecular Forces

Intermolecular forces are attractive forces between molecules.

Intramolecular forces hold atoms together in a molecule.

Intermolecular vs Intramolecular

• 41 kJ to vaporize 1 mole of water (inter)

• 930 kJ to break all O-H bonds in 1 mole of water (intra)

Generally, intermolecular forces are much weaker than intramolecular forces.

“Measure” of intermolecular force

boiling point

melting point

5

Dipole Moments 01

•Polar covalent bonds form between atoms of different electronegativity. This is described as a bond dipole.

Intermolecular Forces

6

Dipole Moments 02•Dipole Moment (µ): The measure of net molecular polarity or charge separation.

µ = Q r

r = distance between charges

+ = Q, – = –Q

7

Dipole Moments: µ = Q r

• Q = Charge of electron: Q = 1.60 x 10 -19 C,• r = bond length, m• μ , dipole moments are expressed in debyes (D) where

1 D = 3.336 x 10–30 C·m What is the dipole moment if one proton separated from one electron by a distance of 100 PM

μ = Q x r = (1.60 x 10 -19 C) (100 x 10 -12 m) (1D/3.336 x 10-30 C . m) = 4.80 D

8

Dipole Moments 03

•Polarity can be illustrated with an electrostatic potential map. These show electron-rich groups as red and electron-poor groups as blue-green.

9

Dipole Moments 04

11

Intermolecular Forces 01

•Attractive forces between molecules and ions.

•Several types of forces:

–Dipole–dipole

–Instantaneous induced dipole (dispersion forces)

–Ion–dipole

–Hydrogen “bonds.”

12

Intermolecular Forces

Dipole-Dipole Forces

Attractive forces between polar molecules

Orientation of Polar Molecules in a Solid

13

Intermolecular Forces

Ion-Dipole Forces

Attractive forces between an ion and a polar molecule

Ion-Dipole Interaction

14

Intermolecular Forces 04

•London Dispersion Forces: Attraction is due to instantaneous, temporary dipoles formed due to electron motions.

15

Intermolecular ForcesDispersion Forces Continued

Polarizability is the ease with which the electron distribution in the atom or molecule can be distorted.

Polarizability increases with:

• greater number of electrons

• more diffuse electron cloud

Dispersion forces usually increase with molar mass.

2XXXXX XXXX

16

SO

O

What type(s) of intermolecular forces exist between each of the following molecules?

HBrHBr is a polar molecule: dipole-dipole forces. There are also dispersion forces between HBr molecules.

CH4

CH4 is nonpolar: dispersion forces.

SO2

SO2 is a polar molecule: dipole-dipole forces. There are also dispersion forces between SO2 molecules.

17

Hydrogen Bond

•Hydrogen Bond: Molecules containing N–H, O–H, or F–H groups, and an electronegative O, N, or F.

18

Why is the hydrogen bond considered a “special” dipole-dipole interaction?

Decreasing molar massDecreasing boiling point

19

Which of the following molecules can hydrogen bond with itself?

• 1, 2• 2, 3• 3, 4• 1, 2, 3• 1, 2, 3, 4

CH2F2 NH3 CH3-O-H CH3C CH3

O

1 2 3 4

20

Which of the following molecules can hydrogen bond with itself?

• 1, 2• 2, 3• 3, 4• 1, 2, 3• 1, 2, 3, 4

CH2F2 NH3 CH3-O-H CH3C CH3

O

1 2 3 4

21

Of the following substances, predict which has the lowest boiling point based on London dispersion forces.

1. He2. Ne3. Ar4. Kr5. Xe

22

Correct Answer:

More massive species have more polarizability and stronger London dispersion forces; consequently, amongst the noble gases He has the lowest boiling point.

1. He2. Ne3. Ar4. Kr5. Xe

23

Of the following substances, predict which has the highest boiling point based upon intermolecular forces?

1. CH4

2. H2O3. H2S4. SiH4

5. H2Se

NH ……. O=C

24

Correct Answer:

Of these, only H2O has any hydrogen bonding. Hydrogen bonding substantially increases the intermolecular forces, and hence the boiling point.

1. CH4

2. H2O3. H2S4. SiH4

5. H2Se

25

With nerves as steady as a chemical bond.

© 2003 John Wiley and Sons Publishers

Courtesy Ken Karp

26Figure 13.1: “Floating” a tack on water.

© 2003 John Wiley and Sons Publishers

27Figure 13.2: Place a tack on the surface of a glass of water.

© 2003 John Wiley and Sons Publishers

Courtesy Ken Karp

28

Surface Tension

Water strider walks on a pond without penetrating the surface

29

Surface Tension

30

Properties of Liquids

Surface tension is the amount of energy required to stretch or increase the surface of a liquid by a unit area.

Strong intermolecular

forces

High surface tension

31

Viscosity

Viscosity is the measure of a liquid’s resistance to flow and is related to the ease with which molecules move around, and thus to the intermolecular forces.

32

Surface Tension

Tensiometer

33

Intermolecular Forces 09•Viscosity is the measure of a liquid’s resistance to flow and is related to the ease with which molecules move around, and thus to the intermolecular forces.

Another unit of viscosity is kg/m.s

34

Phase Changes 01

Phase ChangesPhase Change (State Change): A change in physical form but not the chemical identity of a substance.

liquid to solid

gas to liquid

gas to solid

Freezing:

Condensation:

Deposition:

solid to liquid

liquid to gas

solid to gas

Fusion (melting):

Vaporization :

Sublimation:

36

Phase Changes 02

kJ/mol (∆Hvap )(∆Hfus)

(∆Hfus) = 6.01 KJ/mol (∆Hvap ) = 40.67 KJ/mol

37

Phase Changes

• Vapor Pressure: The pressure exerted by gaseous molecules above a liquid.

38

Molar heat of vaporization (Hvap) is the energy required to vaporize 1 mole of a liquid.

ln P = -Hvap

RT+ C

Clausius-Clapeyron EquationP = (equilibrium) vapor pressure

T = temperature (K)

R = gas constant (8.314 J/K•mol)

39

Vapor Pressure

• The boiling point of a liquid is the temperature at which its vapor pressure equals atmospheric pressure.

• The normal boiling point is the temperature at which its vapor pressure is 760 torr.

Evaporation, Vapor Pressure, and Boiling Point

+ C1

T-

Hvap

Rln Pvap =

m x b+y =

Evaporation, Vapor Pressure, and Boiling Point

Vapor Pressure

42

43

•By taking measurements at two temps, we get:

12

vap

2

1 11ln

TTR

H

PP

ln P = -Hvap

RT+ C

Clausius-Clapeyron Equation

44

The normal boiling point of benzene is 80.1 °C, and ΔHvap = 30.8 kJ/mol, what is boiling point of benzene on top of Mount Everest, where P = 260 mm Hg

• P1 = 760 mm Hg; P2 = 260 mm Hg; t1 = 80.1oC, T2 = ?

• ΔHvap = 30.8 kJ/mol

• , R = 8.3145 J / K . mol

• Solve for T2 (the boiling point for benzene at 260 mm Hg).

T2 = 320 K ; t = 47oC

(boiling point is lower at lower pressure)

12

vap

2

1 11ln

TTR

H

PP

45

Which statement is

true? • Boiling point ~120°C• Boiling point ~95°C • Boiling point ~75°C• Melting point ~95°C• Melting point ~75°C

0

200

400

600

800

Vap

or

Pre

ssu

re (

mm

Hg

)

25 50 75 100Temperature (° C)

0

46

Which statement is

true? • Boiling point ~120°C• Boiling point ~95°C • Boiling point ~75°C• Melting point ~95°C• Melting point ~75°C

0

200

400

600

800

Vap

or

Pre

ssu

re (

mm

Hg

)

25 50 75 100Temperature (° C)

0

47

An amorphous solid does not possess a well-defined arrangement and long-range molecular order they do not have a fixed sharp melting point. .

A glass is an optically transparent fusion product of inorganic materials that has cooled to a rigid state without crystallizing

Crystallinequartz (SiO2)

Non-crystallinequartz glass

Solids

•Structure of a crystalline solid is based on the unit cell, a basic

• repeating structural unit.

Kinds of SolidsAmorphous Solids: Particles are randomly arranged and have no ordered long-range structure. Example - rubber.

Crystalline Solids: Particles have an ordered arrangement extending over a long range.

• ionic solids• molecular solids• covalent network solids• metallic solids

Kinds of Solids

Ionic Solids: Particles are ions ordered in a regular three-dimensional arrangement and held together by ionic bonds. Example - sodium chloride.

50

Unit Cell

latticepoint

Unit cells in 3 dimensions

At lattice points:

• Atoms

• Molecules

• Ions

Simple CubicPacking

Body-Centered CubicPacking

52

Crystal StructureSimple CubeSimple Cube Body-Centered Cube:Body-Centered Cube:

53

Crystal Structure 04

Face-Centered Cube:Face-Centered Cube:

54

Crystalline SolidsWe can determine the empirical formula of an ionic solid by determining how many ions of each element fall within the unit cell.

Hexagonal Closest Pack

A-B-A-B- Space used 74%

Cubic Closes Pack

• Space used 74%

• A-B-C-A-B-C

56

57

Unit Cells and the Packing of Spheres in Crystalline Solids

Unit Cell: A small repeating unit that makes up a crystal.

59

Types of Crystals

What are the empirical formulas for these compounds?(a) Orange:chlorine; Gray:cesium(b) Blue:sulfur; Gray: zinc(c) Green:fluorine, Gray: calcium

CsCl ZnS CaF2

(a) (b) (c)

60

Types of Crystal 04

•Carbon:

Carbon Allotropes

62

Types of Crystals

Covalent Crystals• Lattice points occupied by atoms• Held together by covalent bonds• Hard, high melting point

diamond graphite

carbonatoms

lattice points:

• Atoms

• Molecules

• Ions

63

Types of Crystals

Molecular Crystals• Lattice points occupied by molecules• Held together by intermolecular forces• Soft, low melting point

11.6

64

Types of Crystals

Metallic Crystals• Lattice points occupied by metal atoms• Held together by metallic bonds• Soft to hard, low to high melting point• Good conductors of heat and electricity

Cross Section of a Metallic Crystal

nucleus &inner shell e-

mobile “sea”of e-

65

• Ionic Crystals• Covalent Crystals• Molecular Crystals• Metallic Crystals

66Body-centered cubic Face-centered cubicSimple cubic cell

67

When silver crystallizes, it forms face-centered cubic cells. The unit cell edge length is 409 pm. Calculate the density of silver.

d = mV

V = a3 = (409 pm)3 = 6.83 x 10-23 cm3

4 atoms/unit cell in a face-centered cubic cell

m = 4 Ag atoms107.9 gmole Ag

x1 mole Ag

6.022 x 1023 atomsx = 7.17 x 10-22 g

d = mV

7.17 x 10-22 g6.83 x 10-23 cm3

= = 10.5 g/cm3

68

X-Ray Crystallography

• Diffraction is the scattering of radiation by an object containing regularly spaced lines, with a spacing that is equivalent to the wavelength of radiation.

• Diffraction is due to interference between two waves passing through the same region of space at the same time.

69

70Extra distance = BC + CD = 2d sin = n (Bragg Equation)

71

X rays of wavelength 0.154 nm are diffracted from a crystal at an angle of 14.170. Assuming that n = 1, what is the distance (in pm) between layers in the crystal?

n = 2d sin n = 1 = 14.170 = 0.154 nm = 154 pm

d =n

2sin=

1 x 154 pm

2 x sin14.17= 315 pm

72

Titanium metal has a density of 4.54 g/cm3, and an atomic radius of 144.8 pm. What is the structure of cubic unit cell?

• mass of one Ti atom = 7.951 x 10 -23 g/atom (problem 10.78)

• r = 144.8 pm = 144.8 x 10 -12 m• r = 144.8 x 10 -12 m = 1.448 x 10 -8 cm• Calculate the volume and then the density for Ti assuming

it is Simple (primitive) cubic, body-centered cubic, and face-centered cubic. Compare the calculated density with the actual density to identify the unit cell.

• For primitive cubic:• a = 2r; volume = a3 = [2(1.448 x 10 -8 cm)]3 = 2.429 x 10 -23

cm3

• density = m/v = 3.273 g/cm3

atoms 10 x 6.022

mol 123

73

• For face-centered cubic:• a = √8. r; volume = a3 = [2√2 . (1.448 x 10- 8

cm)]3 = 6.870 x 10 -23 cm3

• density = = 4.630 g/cm3

• For body-centered cubic:• a = 4r/√3; volume = a3 = 3.739 x 10 23 cm3

• density = = 4.253 g/cm3• The calculated density for a face-centered cube

(4.630 g/cm3) is closest to the actual density of 4.54 g/cm3. Ti crystallizes in the face-centered cubic unit cell.

74

Phase Diagrams 01

Water

Phase Diagrams

Normal BP: Occurs at 1 atm.

Critical Point: A combination of temperature and pressure beyond which a gas cannot be liquefied.

• Critical Temperature: The temperature beyond which a gas cannot be liquefied regardless of the pressure.

• Critical Pressure: The pressure beyond which a liquid cannot be vaporized regardless of the temperature.

Supercritical Fluid: A state of matter beyond the critical point that is neither liquid nor gas.

Triple Point: A point at which three phases coexist in equilibrium.

Supercritical CO2

77

Caffeine extraction from green coffee with supercritical CO2

Application of Supercritical CO2 in dry cleaning

Phase DiagramsCarbon Dioxide

79

Phase Diagrams 05

• Approximately, what is the normal boiling point and what is the normal melting point of the substance?

• What is the physical state when:i. T = 150 K, P = 0.5 atm

ii. T = 325 K, P = 0.9 atm

iii. T = 450 K, P = 265 atm

The End

80

Coordination Numbers

81

82

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