Structures of Metals and Ceramics

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MSE 528

Fall 2010

Atomic Structure and

Interatomic Bonding

ISSUES TO ADDRESS...

• What promotes bonding?

• What types of bonds are there?

• What properties are inferred from bonding?

1

BOHR ATOM

orbital electrons: n = principal quantum number n=3 2

1

Adapted from Fig. 2.1,

Callister 6e.

Nucleus: Z = # protons

= 1 for hydrogen to 94 for plutonium

N = # neutrons

Atomic mass A ≈ Z + N

2

ELECTRON ENERGY STATES

Electrons...

• have discrete energy states

• tend to occupy lowest available energy state.

Adapted from Fig. 2.5,

Callister 6e.

3

STABLE ELECTRON CONFIGURATIONS

Stable electron configurations...

• have complete s and p subshells

• tend to be unreactive .

Adapted from Table 2.2,

Callister 6e.

4

SURVEY OF ELEMENTS

• Most elements: Electron configuration not stable .

Electron configuration

1s 1

1s 2 (stable)

1s 2 2s 1

1s 2 2s 2

1s 2 2s 2 2p 1

1s 2 2s 2 2p 2

...

1s 2 2s 2 2p 6 (stable)

1s 2 2s 2 2p 6 3s 1

1s 2 2s 2 2p 6 3s 2

1s 2 2s 2 2p 6 3s 2 3p 1

...

Adapted from Table 2.2,

Callister 6e.

1s 2 2s 2 2p 6 3s 2 3p 6

...

(stable)

1s 2 2s 2 2p 6 3s 2 3p 6 3d 10 4s 2 4 6 (stable)

• Why? Valence (outer) shell usually not filled completely.

5

THE PERIODIC TABLE

• Columns: Similar Valence Structure

Adapted from Fig. 2.6,

Callister 6e.

Electropositive elements:

Readily give up electrons to become + ions.

Electronegative elements:

Readily acquire electrons to become - ions.

6

ELECTRONEGATIVITY

• Ranges from 0.7

to 4.0

,

• Large values: tendency to acquire electrons.

Smaller electronegativity Larger electronegativity

Adapted from Fig. 2.7, Callister 6e. (Fig. 2.7 is adapted from Linus Pauling, The Nature of the

Chemical Bond, 3rd edition, Copyright 1939 and 1940, 3rd edition. Copyright 1960 by Cornell

University.

7

IONIC BONDING

• Occurs between + and - ions.

• Requires electron transfer.

• Large difference in electronegativity required.

• Example: NaCl

8

EXAMPLES: IONIC BONDING

• Predominant bonding in Ceramics

Be

1.5

Mg

1.2

Ca

1.0

Sr

1.0

Ba

0.9

Ra

0.9

H

2.1

Li

1.0

Na

0.9

K

0.8

Rb

0.8

Cs

0.7

Fr

0.7

Ti

1.5

Cr

1.6

Fe

1.8

NaCl

MgO

CaF2

CsCl

Ni

1.8

Zn

1.8

As

2.0

O

3.5

F

4.0

Cl

3.0

Br

2.8

I

2.5

At

2.2

He

-

Ne

-

Ar

-

Kr

-

Xe

-

Rn

-

Give up electrons Acquire electrons

Adapted from Fig. 2.7, Callister 6e. (Fig. 2.7 is adapted from Linus Pauling, The Nature of the

Chemical Bond, 3rd edition, Copyright 1939 and 1940, 3rd edition. Copyright 1960 by Cornell

University.

9

COVALENT BONDING

• Requires shared electrons

• Example: CH

4

C: has 4 valence e, needs 4 more

H: has 1 valence e, needs 1 more

Electronegativities are comparable.

Adapted from Fig. 2.10, Callister 6e.

10

Rb

0.8

Cs

0.7

Fr

0.7

H

2.1

Li

1.0

Na

0.9

K

0.8

Be

1.5

Mg

1.2

Ca

1.0

Sr

1.0

Ba

0.9

Ra

0.9

EXAMPLES: COVALENT BONDING

H2O

H2

C(diamond)

SiC

Ti

1.5

Cr

1.6

Fe

1.8

Ni

1.8

Zn

1.8

Ga

1.6

C

2.5

Si

1.8

Ge

1.8

Sn

1.8

Pb

1.8

As

2.0

GaAs

O

2.0

F

4.0

Cl

3.0

Br

2.8

I

2.5

At

2.2

He

-

Ne

-

Ar

-

Kr

-

Xe

-

Rn

-

F2

Cl2

• Molecules with nonmetals

• Molecules with metals and nonmetals

• Elemental solids (RHS of Periodic Table)

• Compound solids (about column IVA )

11

METALLIC BONDING

• Arises from a sea of donated valence electrons

(1, 2, or 3 from each atom).

Adapted from Fig. 2.11, Callister 6e.

• Primary bond for metals and their alloys

12

SECONDARY BONDING

Arises from interaction between dipoles

• Fluctuating dipoles

Adapted from Fig. 2.13, Callister 6e.

• Permanent dipoles -molecule induced

-general case:

-ex: liquid HCl

-ex: polymer

Adapted from Fig. 2.14,

Callister 6e.

Adapted from Fig. 2.14,

Callister 6e.

13

Type

Ionic

SUMMARY: BONDING

Bond Energy

Large!

Comments

Nondirectional ( ceramics )

Covalent

Metallic

Secondary

Variable large-Diamond small-Bismuth

Directional semiconductors , ceramics polymer chains)

Variable large-Tungsten small-Mercury smallest

Nondirectional ( metals

Directional inter-chain ( polymer ) inter-molecular

)

14

PROPERTIES FROM BONDING: T

M

• Bond length , r

• Melting Temperature , T m

F r

• Bond energy , E o

F

T m is larger if E o is larger.

15

PROPERTIES FROM BONDING: E

• Elastic modulus , E

Elastic modulus

F

A o

= E

 L

L o

• E ~ curvature at r o

Energy unstretched length r o r

E is larger if E smaller Elastic Modulus o is larger.

larger Elastic Modulus

16

PROPERTIES FROM BONDING:

a

• Coefficient of thermal expansion , a coeff. thermal expansion

 L

Lo

 = a ( T

2

T

1

)

• a ~ symmetry at r o a is larger if E o is smaller.

17

SUMMARY: PRIMARY BONDS

Ceramics

(Ionic & covalent bonding):

Large bond energy large T m large E small a

Metals

(Metallic bonding):

Variable bond energy moderate T m moderate E moderate a

Polymers

(Covalent & Secondary):

Directional Properties

Secondary bonding dominates small T small E large a

18

Structures of Metals and

Ceramics

ISSUES TO ADDRESS...

• How do atoms assemble into solid structures?

• How do the structures of ceramic materials differ from those of metals?

• How does the density of a material depend on its structure?

• When do material properties vary with the sample (i.e., part) orientation?

1

ENERGY AND PACKING

• Non dense, random packing

• Dense, regular packing

Dense, regular-packed structures tend to have lower energy.

2

METALLIC CRYSTALS

• tend to be densely packed.

• have several reasons for dense packing:

-Typically, only one element is present, so all atomic radii are the same.

-Metallic bonding is not directional.

-Nearest neighbor distances tend to be small in order to lower bond energy.

• have the simplest crystal structures.

We will look at three such structures...

3

SIMPLE CUBIC STRUCTURE (SC)

• Rare due to poor packing (only Po has this structure)

• Close-packed directions are cube edges.

• Coordination # = 6

(# nearest neighbors)

Click on image to animate

(Courtesy P.M. Anderson)

4

ATOMIC PACKING FACTOR

• APF for a simple cubic structure = 0.52

Adapted from Fig. 3.19,

Callister 6e.

5

FACE CENTERED CUBIC STRUCTURE

(FCC)

• Close packed directions are face diagonals.

--Note: All atoms are identical; the face-centered atoms are shaded differently only for ease of viewing.

• Coordination # = 12

Click on image to animate

(Courtesy P.M. Anderson)

Adapted from Fig. 3.1(a),

Callister 6e.

6

ATOMIC PACKING FACTOR: FCC

• APF for a body-centered cubic structure = 0.74

Unit cell contains:

6 x 1/2 + 8 x 1/8

= 4 atoms/unit cell a

Adapted from

Fig. 3.1(a),

Callister 6e.

7

BODY CENTERED CUBIC STRUCTURE

(BCC)

• Close packed directions are cube diagonals.

--Note: All atoms are identical; the center atom is shaded differently only for ease of viewing.

• Coordination # = 8

Click on image to animate

(Courtesy P.M. Anderson)

Adapted from Fig. 3.2,

Callister 6e.

8

ATOMIC PACKING FACTOR: BCC

• APF for a body-centered cubic structure = 0.68

Adapted from

Fig. 3.2,

Callister 6e.

R a

Unit cell contains:

1 + 8 x 1/8

= 2 atoms/unit cell

9

HEXAGONAL CLOSE-PACKED

STRUCTURE (HCP)

• ABAB... Stacking Sequence

• 3D Projection • 2D Projection

A sites

B sites

A sites

Adapted from Fig. 3.3,

Callister 6e.

• Coordination # = 12

• APF = 0.74

10

THEORETICAL DENSITY,

Example: Copper

Data from Table inside front cover of Callister (see next slide):

• crystal structure = FCC: 4 atoms/unit cell

• atomic weight = 63.55 g/mol (1 amu = 1 g/mol)

• atomic radius R = 0.128 nm (1 nm = 10 cm)

Result: theoretical 

Cu = 8.89 g/cm3

Compare to actual: 

Cu = 8.94 g/cm3

11

Characteristics of Selected Elements at 20C

Element

Aluminum

Argon

Barium

Beryllium

Boron

Bromine

Cadmium

Calcium

Carbon

Cesium

Chlorine

Chromium

Cobalt

Copper

Flourine

Gallium

Germanium

Gold

Helium

Hydrogen

Cu

F

Ga

Ge

Au

He

H

Br

Cd

Ca

C

Cs

Cl

Cr

Co

Symbol

Al

Ar

Ba

Be

B

At. Weight

(amu)

26.98

39.95

137.33

9.012

10.81

79.90

112.41

40.08

12.011

132.91

35.45

52.00

58.93

63.55

19.00

69.72

72.59

196.97

4.003

1.008

Density

1.87

------

7.19

8.9

8.94

------

5.90

(g/cm3)

2.71

------

3.5

1.85

2.34

------

8.65

1.55

2.25

5.32

19.32

------

------

Atomic radius

(nm)

0.143

------

0.217

0.114

------

------

0.149

0.197

0.071

Adapted from

Table, "Characteristics of

Selected

Elements", inside front cover,

Callister 6e.

0.265

------

0.125

0.125

0.128

------

0.122

0.122

0.144

------

------

12

DENSITIES OF MATERIAL CLASSES

 metals

•  ceramics

•  polymers

Why?

Metals have...

• close-packing

(metallic bonding)

• large atomic mass

Ceramics have...

• less dense packing

(covalent bonding)

• often lighter elements

Polymers have...

• poor packing

(often amorphous)

• lighter elements (C,H,O)

Composites have...

• intermediate values

Data from Table B1, Callister 6e.

13

CERAMIC BONDING

• Bonding:

--Mostly ionic, some covalent.

--% ionic character increases with difference in electronegativity.

• Large vs small ionic bond character:

Adapted from Fig. 2.7, Callister 6e. (Fig. 2.7 is adapted from Linus Pauling, The Nature of the

Chemical Bond, 3rd edition, Copyright 1939 and 1940, 3rd edition. Copyright 1960 by

Cornell University.

14

IONIC BONDING & STRUCTURE

• Charge Neutrality :

--Net charge in the structure should be zero.

--General form:

• Stable structures:

--maximize the # of nearest oppositely charged neighbors.

Adapted from Fig. 12.1,

Callister 6e.

15

COORDINATION # AND IONIC RADII

• Coordination # increases with

Issue: How many anions can you arrange around a cation?

Adapted from Fig. 12.4,

Callister 6e.

Adapted from Table

12.2, Callister 6e.

Adapted from Fig. 12.2,

Callister 6e.

Adapted from Fig. 12.3,

Callister 6e.

16

EX: PREDICTING STRUCTURE OF FeO

• On the basis of ionic radii, what crystal structure would you predict for FeO?

Cation

Al3+

Fe2+

Fe3+

Ca2+

Anion

O2-

Cl-

F-

• Answer: r r cation

Data from Table 12.3,

Callister 6e.

anion

0.077

0.140

0.550

based on this ratio,

--coord # = 6

--structure = NaCl

17

A

m

X

p

STRUCTURES

• Consider CaF

2

: r cation r anion

0.100

0.133

0.8

• Based on this ratio, coord # = 8 and structure = CsCl.

• Result: CsCl structure w/only half the cation sites occupied.

• Only half the cation sites are occupied since

#Ca 2+ ions = 1/2 # F ions.

Adapted from Fig. 12.5,

Callister 6e.

18

DEMO: HEATING AND

COOLING OF AN IRON WIRE

• Demonstrates " polymorphism "

The same atoms can have more than one crystal structure.

19

FCC STACKING SEQUENCE

• ABCABC... Stacking Sequence

• 2D Projection

A

A

B

C

B

A sites B

C

B

C

B

B sites B B

C sites

• FCC Unit Cell

20

STRUCTURE OF COMPOUNDS: NaCl

• Compounds: Often have similar close-packed structures.

• Structure of Na Cl • Close-packed directions

--along cube edges.

Click on image to animate

(Courtesy P.M. Anderson)

Click on image to animate

(Courtesy P.M. Anderson)

21

CRYSTALS AS BUILDING BLOCKS

• Some engineering applications require single crystals:

--diamond single --turbine blades crystals for abrasives

(Courtesy Martin Deakins,

GE Superabrasives,

Worthington, OH. Used with permission.)

Fig. 8.30(c), Callister 6e.

(Fig. 8.30(c) courtesy of Pratt and Whitney).

• Crystal properties reveal features of atomic structure.

--Ex: Certain crystal planes in quartz fracture more easily than others.

(Courtesy P.M. Anderson)

22

POLYCRYSTALS

• Most engineering materials are polycrystals.

Adapted from Fig. K, color inset pages of

Callister 6e.

(Fig. K is courtesy of

Paul E. Danielson,

Teledyne Wah Chang

Albany)

1 mm

• Nb-Hf-W plate with an electron beam weld.

• Each "grain" is a single crystal.

• If crystals are randomly oriented, overall component properties are not directional.

• Crystal sizes typ. range from 1 nm to 2 cm

(i.e., from a few to millions of atomic layers).

23

SINGLE VS POLYCRYSTALS

• Single Crystals

-Properties vary with direction: anisotropic .

-Example: the modulus of elasticity (E) in BCC iron:

Data from Table 3.3,

Callister 6e.

(Source of data is

R.W. Hertzberg,

Deformation and

Fracture Mechanics of

Engineering Materials,

3rd ed., John Wiley and Sons, 1989.)

• Polycrystals

-Properties may/may not vary with direction.

-If grains are randomly oriented: isotropic .

(E poly iron

= 210 GPa)

-If grains are textured , anisotropic.

200 m m

Adapted from Fig.

4.12(b), Callister 6e.

(Fig. 4.12(b) is courtesy of L.C. Smith and C. Brady, the

National Bureau of

Standards,

Washington, DC [now the National Institute of Standards and

Technology,

Gaithersburg, MD].)

24

X-RAYS TO CONFIRM CRYSTAL

STRUCTURE

• Incoming X-rays diffract from crystal planes.

Adapted from Fig.

3.2W, Callister 6e.

• Measurement of:

Critical angles, q c

, for X-rays provide atomic spacing, d.

25

MATERIALS AND PACKING

Crystalline materials...

• atoms pack in periodic, 3D arrays

• typical of: -metals

-many ceramics

-some polymers crystalline SiO

2

Adapted from Fig. 3.18(a),

Callister 6e.

Noncrystalline materials...

• atoms have no periodic packing

• occurs for: -complex structures

-rapid cooling

" Amorphous " = Noncrystalline noncrystalline SiO

2

Adapted from Fig. 3.18(b),

Callister 6e.

26

GLASS STRUCTURE

• Basic Unit:

Si4+

O2-

• Glass is amorphous

• Amorphous structure occurs by adding impurities

(Na + ,Mg 2+ ,Ca 2+ , Al 3+ )

• Impurities: interfere with formation of crystalline structure.

• Quartz is crystalline

SiO

2

:

(soda glass)

Adapted from Fig. 12.11,

Callister, 6e.

28

SUMMARY

• Atoms may assemble into crystalline or amorphous structures.

• We can predict the density of a material, provided we know the atomic weight , atomic radius , and crystal geometry (e.g., FCC,

BCC, HCP).

• Material properties generally vary with single crystal orientation (i.e., they are anisotropic ), but properties are generally non-directional

(i.e., they are isotropic ) in polycrystals with randomly oriented grains.

27

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