Solid State

142
Solid State Gases: no definite shape and volume Solids: definite shape, volume and order. Order: definite pattern of arrangement of atoms or molecules or ions. Liquids: no definite shape but definite vol Solids: definite shape and volume

description

 

Transcript of Solid State

Page 1: Solid State

Solid StateSolid StateGases: no definite shape and volume

Solids: definite shape, volume and order.

Order: definite pattern of arrangement of atoms or molecules or ions.

Liquids: no definite shape but definite volume

Solids: definite shape and volume

Page 2: Solid State

Intensive properties: do not depend on the amount.

Unit Cells

• Smallest Repeating Unit

• Unit Cells must link-up cannot have gaps between them

• All unit cells must be identical

Page 3: Solid State
Page 4: Solid State

Choice of the origin is arbitrary

Page 5: Solid State

Blue atom or orange atom or

Page 6: Solid State

even a space!

Page 7: Solid State

This cannot be a unit cell

Unit cells are not identical

Page 8: Solid State

This also cannot be a unit cell

Space between unit cells not allowed

Page 9: Solid State

Unit cells exist in only seven shapes

Cubic

Orthorhombic

Rhombohedral

Tetragonal

Triclinic

Hexagonal

Monoclinic

Page 10: Solid State

Crystal intercepts & Angles

a

b

c

Page 11: Solid State

Crystal Systems

Lattice Parameters

Crystal Intercepts Crystal Angles

Cubic a = b = c = = = 90o

Orthorhombic a b c = = = 90o

Rhombohedral a = b = c = = 90o

Tetragonal a = b c = = = 90o

Triclinic a b c 90o

Hexagonal a = b c = = 90o,

= 120o

Monoclinic a b c = = 90o,

90o

Page 12: Solid State

There are not more than 4 ways of arranging spheres in any shape of unit cell

These are Primitive, Body Centered, Face Centered & End Centered

Page 13: Solid State

a = 2r

1

2

4

3

5

67

8

Unit Cell shape view

Unit Cell arrangement view

Page 14: Solid State

Layer arrangement view

Page 15: Solid State
Page 16: Solid State

Volume occupied by a sphere in the unit cell V81

Total volume occupied by all the spheres in the unit cell

VV 1881

Page 17: Solid State

Packing Fraction

Fraction of the Unit cell’s volume occupied by the spheres

cellunitofvolume

cellunittheinsidespheresthebyoccupiedVolume

3

3

34

a

r

3

3

234

r

r

52.0

Page 18: Solid State

Coordination number

6

Page 19: Solid State

Unit Cell shape view

Unit Cell arrangement view

Page 20: Solid State

Layer arrangement view

Page 21: Solid State

ar 34

23

2a

r a

a > 2r

Page 22: Solid State
Page 23: Solid State

Packing Fraction

3

3

3434

2

r

r

68.0

Volume occupied by a corner sphere in the unit cell V81

Volume occupied by the central sphere in the unit cell V1

Total Volume occupied by the spheres in the unit cell

V2

Packing Fraction

Page 24: Solid State

Coordination number

8

Page 25: Solid State

Unit Cell shape view

Unit Cell arrangement view

Page 26: Solid State

a

ar 24

22

ar a

r2

Page 27: Solid State
Page 28: Solid State

Packing Fraction

3

3

2434

4

r

r

74.0

Volume occupied by a corner sphere in the unit cell V81

Volume occupied by a face centered sphere in the unit cell

V21

Total Volume occupied by the spheres in the unit cell 4

21

681

8

Packing Fraction

Highest Packing Fraction of all shapes and of all arrangements

Page 29: Solid State

Coordination number

x y

z

y-z plane

x-z plane x-y plane

Page 30: Solid State

Coordination number

a/2

a/2

2a

Page 31: Solid State
Page 32: Solid State

Out of all the twenty eight possible unit cells only 14 exist !

Those arrangements in a given shape that violate even one symmetry element of that shape do not exist in that shape

90o axis of symmetry

Page 33: Solid State
Page 34: Solid State
Page 35: Solid State
Page 36: Solid State
Page 37: Solid State
Page 38: Solid State
Page 39: Solid State
Page 40: Solid State
Page 41: Solid State
Page 42: Solid State
Page 43: Solid State
Page 44: Solid State
Page 45: Solid State
Page 46: Solid State
Page 47: Solid State
Page 48: Solid State
Page 49: Solid State
Page 50: Solid State
Page 51: Solid State
Page 52: Solid State
Page 53: Solid State
Page 54: Solid State
Page 55: Solid State
Page 56: Solid State
Page 57: Solid State
Page 58: Solid State
Page 59: Solid State
Page 60: Solid State
Page 61: Solid State
Page 62: Solid State
Page 63: Solid State
Page 64: Solid State

If we do the same with BCC & FCC we will get the same result.

Lets try with End Centered

Page 65: Solid State
Page 66: Solid State
Page 67: Solid State
Page 68: Solid State
Page 69: Solid State
Page 70: Solid State
Page 71: Solid State
Page 72: Solid State
Page 73: Solid State
Page 74: Solid State
Page 75: Solid State
Page 76: Solid State
Page 77: Solid State
Page 78: Solid State
Page 79: Solid State
Page 80: Solid State
Page 81: Solid State
Page 82: Solid State
Page 83: Solid State
Page 84: Solid State
Page 85: Solid State
Page 86: Solid State
Page 87: Solid State
Page 88: Solid State
Page 89: Solid State
Page 90: Solid State
Page 91: Solid State

Like this 13 other arrangements in various shapes were rejected.

We are left with only 14 unit cells

Page 92: Solid State

Crystal Systems

Cubic

Orthorhombic

Rhombohedral

Tetragonal

Triclinic

Hexagonal

Monoclinic

Bravais Lattices

Primitive, FCC, BCC

Primitive, FC, BC, EC

Primitive

Primitive, BC

Primitive

Primitive

Primitive, EC

Page 93: Solid State

Layer A

Layer arrangement view

Page 94: Solid State

Layer B

Page 95: Solid State

Layer C

Layer A

Layer B

Layer C

Cubic Close Packing(CCP)

Page 96: Solid State
Page 97: Solid State

Layer A

Layer arrangement view

Page 98: Solid State

Layer B

Page 99: Solid State

Layer A

Layer A

Layer B

Layer A

Hexagonal Close Packing

Page 100: Solid State

Unit Cell shape view

Unit Cell arrangement view

Page 101: Solid State

a

c

a = 2r

2r2r

2r

r

O

A

B

30

o

OA = rAOB = 30o

BDr

OB 3

2

O

B

c/2DD

E

2r

232

23

2)2(

22 c

rr

rEB

32

4rc

Page 102: Solid State

Contribution of corner atom61

Contribution of Face atom21

Contribution of second layeratoms

3

Total atoms per unit cell 6

Page 103: Solid State

Packing Fraction

32

4243

6

34

6

2

3

rr

r

2243

6 r32

4r

74.0

Page 104: Solid State

Packing Fraction depends on:

1. Layout of each layer

2. Placement of one layer over the other

Page 105: Solid State

r 30

o

O

AB

AB = r

OA = r tan30o

3r

< r

Packing Fraction same

Rank of unit cell 2Volume of unit cell 1/3 of previous

mass of unit cell 1/3 of previous

density same

Page 106: Solid State
Page 107: Solid State

Two types of voids:

Octahedral

Tetrahedral

Found only in FCC & Hexagonal primitive unit cells

Octahedral void in FCC

Page 108: Solid State

Each octahedral void located at the edge center is shared by 4 unit cells

Total contribution of edge centre voids = 31241

Contribution of central void 1

Total contribution of all octahedral voids per unit cell of FCC = 4

No. of Octahedral voids per unit cell = Rank of unit cell

Page 109: Solid State

Tetrahedral void in FCC

(0,0,0) x-axis

y-axis

z-axis

(a/2, a/2,0)

(a/2, 0,a/2)(0, a/2,a/2)

(a/4, a/4,a/4)

Page 110: Solid State

(0,0,0)

(a/2, a/2,0)

(a/4, a/4,a/4)a

b

ka

ja

ia

a ˆ4

ˆ4

ˆ4

ka

ja

ia

b ˆ4

ˆ4

ˆ4

ba

ba

.

.cos1

163

16cos 2

2

1

a

a

31

cos1 o268.109

Page 111: Solid State

With each corner as origin there are 8 tetrahedral voids in FCC unit cell

No. of tetrahedral voids = 2 no. of Octahedral voids

Page 112: Solid State

Voids in Hexagonal Primitive

Let us assume that this is the unit cell

then according to what we have done in FCC no. of Octahedral voids = 6 & no. of tetrahedral voids = 12

Octahedral voids

Octahedral void

Page 113: Solid State

Voids in Hexagonal Primitive

Let us assume that this is the unit cell

then according to what we have done in FCC no. of Octahedral voids = 6 & no. of tetrahedral voids = 12

Tetrahedral voids

Contribution of tetrahedral voids formed inside the unit cell is 1 each. The ones formed on the corners of the hexagon have a contribution of 1/3.Total contribution 66

31

4

In 3 layers 1262

Page 114: Solid State

Minimum rc/ra for various coordination numbers

2ra B

O

A

32

30sec

a

ac

r

rr

ABOA

155.0132

a

c

rr

30

o Coordination number - 3

Page 115: Solid State

43

444

222 aaaarrAB ac

ara 42

Coordination number - 4

z-axis

A

B

(0,0,0)

(a/4, a/4,a/4)

24

43 a

ac

rrr

aac rrr23

23

1a

c

rr

225.0123

a

c

rr

Page 116: Solid State

Coordination number - 4 (square planar) or 6 (octahedron)

B

A 2a

rrAB ac

ara 2

aa

ac rr

rr 22

2

414.012 a

c

rr

Page 117: Solid State

Coordination number - 8 (cube)

ac rra

23

ara 2

aca rrr 223

732.013 a

c

rr

Page 118: Solid State

Final Radius Ratios

Radius Ratio, rc/raCo-ordination No.

<0.155 2

[0.155, 0.225) 2 or 3

[0.225, 0.414) 2 or 3 or 4 Td

[0.414, 0.732) 2 or 3 or 4 Td, 4 sq. pl or 6 Oh

[0.732, 0.99) 2 or 3 or 4 Td, 4 sq. pl or 6 Oh

or 8

Page 119: Solid State

For ionic compounds of the general formula AxBy the ratio of the coordination number of A to that of B will be the ratio of y:x.

1. Rock Salt Structure (NaCl) Cl-

Na+

Cl- is FCC

Na+ occupies Octahedral voids

No. of Cl- per unit cell= 4

No. of Na+ per unit cell = 4

formula is NaCl

Coordination no. of Na+ = 6

Coordination no. of Cl- = 6

Page 120: Solid State

Other compounds which have this structure are: all halides of alkali metals except cesium halide, all oxides of alkaline earth metals except beryllium oxide, AgCl, AgBr & AgI.

Page 121: Solid State

Consider the unit cell with Cl- as FCC.

NaClrra 22

Clra 42

Consider the unit cell with Na+ as FCC.

NaClrra 22

Nara 42

Similarly, rany alkali metal = rany halide

ClNarr

rany akaline earth metal = roxide

Comparing

Page 122: Solid State

2. Zinc Blende (ZnS)

S2-

Zn2+

S2- is FCCZn2+ occupies alternate tetrahedral voids

No. of S2- per unit cell= 4

No. of Zn2+ per unit cell = 4

formula is ZnS

Coordination no. of Zn2+ = 4

Coordination no. of S2-= 4

Other compound which have this structure is: BeO

Page 123: Solid State

3. Fluorite (CaF2)

F-

Ca2+

Ca2+ is FCCF- occupies all tetrahedral voids

No. of Ca2+ per unit cell= 4

No. of F- per unit cell= 8

formula is CaF2

Coordination no. of F- = 4

Coordination no. of Ca2+ = 8

Other compounds which have this structure are: UO2, ThO2, PbO2, HgF2 etc.

Page 124: Solid State

4. Anti-Fluorite (Li2O)

O2-

Li+

O2- is FCC Li+ occupies all tetrahedral voids

No. of O2- per unit cell= 4

No. of Li+ per unit cell= 8

formula is Li2O

Coordination no. of Li+ = 4

Coordination no. of O2-= 8

Other compounds which have this structure are: Na2O, K2O, Rb2O

Page 125: Solid State

5. Cesium Halide

Cl-

Cs+

Cl- is Primitive cubic Cs+ occupies the centre of the unit cell

No. of Cl- per unit cell= 1

No. of Cs+ per unit cell= 1

formula is CsCl

Coordination no. of Cs+ = 8

Coordination no. of Cl-= 8

Other compounds which have this structure are: all halides of Cesium and ammonium

Page 126: Solid State

6. Corundum (Al2O3)Oxide ions form hexagonal primitive unit cell and trivalent ions (Al3+) are present in 2/3 of octahedral voids.

No. of O2- per unit cell= 2

No. of Al3+ per unit cell = 4/3

32

64234

OAl

OAl;OAlisformula

Coordination no. of Al3+ = 6

Coordination no. of O2-= 4

Other compounds which have this structure are: Fe2O3, Cr2O3, Mn2O3 etc.

Page 127: Solid State

7. Rutile (TiO2)Oxide ions form hexagonal primitive unit cell and tetravalent ions (Ti4+) are present in 1/2 of octahedral voids.

No. of O2- per unit cell= 2

No. of Ti4+ per unit cell = 1

Coordination no. of Ti4+ = 6

Coordination no. of O2-= 3

Other compounds which have this structure are: MnO2, SnO2, MgF2, NiF2

formula is TiO2

Page 128: Solid State

8. Pervoskite (CaTiO3)

O2-

Ca2+ (divalent ion)

Ca2+ is Primitive cubic

Ti4+ occupies the centre of the unit cell

No. of O2- per unit cell= 3

No. of Ca2+ per unit cell = 1

formula is CaTiO3Coordination no. of O2- = 6

Coordination no. of Ti4+ Other compounds which have this structure are: BaTiO3, SrTiO3

Ti4+ (tetravalent ion)

O2- occupies face centres

No. of Ti4+ per unit cell = 1

= 6

Coordination no. of Ca2+ = 12

Page 129: Solid State

9. Spinel & Inverse Spinel (MgAl2O4)

O2- ion is FCC

Mg2+(divalent ion) 1/8th of tetrahedral voids

Al3+ (trivalent ion) 1/2 of octahedral voids

O2- per unit cell = 4

Mg2+ per unit cell = 1

Al3+ per unit cell = 1

formula is MgAl2O4

Spinel Inverse Spinel

O2- ion is FCCdivalent ion 1/8th of tetrahedral voids

trivalent ion 1/4th of octahedral voids & 1/8th of tetrahedral voids

O2- per unit cell = 4

Divalent per unit cell = 1

Trivalent per unit cell = 1

Page 130: Solid State

(i) Lattice of atoms

(a) Vacancy an atom is missing from its position density decreases

percentage occupancy decreases

100defectwithoutpresentatomsofno.

presentatomsofno.occpancy%

100densityltheoretica

densityobservedoccpancy%

(b) Self interstitial an atom leaves its lattice site & occupies interstitial space density & percentage occupancy remains same

(c) Substitutional impurity foreign atom substitutes a host atom & occupies its lattice density & percentage occupancy may change

(c) Interstitial impurity foreign atom occupies occupies the interstitial space density & percentage occupancy increases

Page 131: Solid State

(i) Ionic structures

(a) Schottky Defect Cation – anion pair are missing

electro neutrality is maintained density decreases

(b) Frenkel Defect ion leaves lattice position & occupies interstitial space electro neutrality is maintained

density maintained(c) Substitutional Impurity Defect Ba2+ is replaced by Sr2+

electro neutrality is maintained density

changes

(d) Interstitial Impurity Defect H2 is trapped in TiC

electro neutrality is maintained density

increases

(a) F-Centre

electron replaces anion electro neutrality is

maintained density decreases colour is imparted

Page 132: Solid State

1. Assuming diamond to be FCC of carbon atoms and that each carbon atom is sp3 hybridized then which of the following statements is correct.

(a) all voids are empty(b) 100% octahedral voids are filled

(c) 50% octahedral voids are filled

(d) 100% tetrahedral voids are filled

(e) 50% tetrahedral voids are filled

Sol: If no void is filled then each carbon would be in contact with 12 carbon atoms. This is not possible as each carbon is sp3 hybridized.

If octahedral voids are filled then those carbons in the voids would be in contact with 6 carbon atoms. This also is not possible.

If 100% tetrahedral voids are filled then the FCC carbons would be in contact with 8 carbon atoms as they are shared in 8 unit cells and would be in contact with 8 tetrahedral voids. Not possible.

(e)

Page 133: Solid State

2. In NaCl calculate:The distance between the first 9 nearest neighbors in a unit cell & their total number in all unit cells

Page 134: Solid State

neighbor no. distance no. of neighbors

12a

6

22a

12

323a 8

4 a 6

525a 24

6 a23 24

7 a2 12

8 a23 24

9 a3 8

Page 135: Solid State

3. Iron crystallizes in FCC lattice. The figures given below shows the iron atoms in four crystallographic planes.

Draw the unit cell for the corresponding structure and identify these planes in the diagram. Also report the distance between two such crystallographic planes in each terms of the edge length ‘a’ of the unit cell.

Page 136: Solid State

distance between two such planes is a

distance between two such planes is a

Page 137: Solid State

distance between two such planes is

A

B

CA

333

distanceaa

2a

Page 138: Solid State

3. Marbles of diameter 10 mm are to be placed on a flat surface bounded by lines of length 40 mm such that each marble has its centre within the bound surface. Find the maximum number of marbles in the bound surface and sketch the diagram. Derive an expression for the number of marbles per unit area.

Interpretation:

1. count marbles as 1 each even if some portion goes outside the bound surface

2. count marbles based on the portion that is inside the bound surface

25

Page 139: Solid State

To calculate no. of marbles per unit area we need to select the smallest repeating unit.

18

d

A B

C

2d43

ABCtriangleofarea

61

3ΔABCinmarblesofno.

0.0115areaunitpermarblesofno.

4103

21

2

18.416000.0115figureenclosedthisinmarblestotalthethisonbased

Page 140: Solid State
Page 141: Solid State
Page 142: Solid State