137
Symmetry in crystals

Symmetry in crystals

Embed Size (px)

DESCRIPTION

Symmetry in crystals. Infinitely repeating lattices. An integral number of unit translations along any axis will arrive at an identical point. A unit translation along any axis will arrive at an identical point. The composition of each unit should be identical. - PowerPoint PPT Presentation

Citation preview

Page 1: Symmetry in crystals

Symmetry in crystals

Page 2: Symmetry in crystals

Infinitely repeating lattices

Page 3: Symmetry in crystals
Page 4: Symmetry in crystals

An integral number of unit translations

along any axis will arrive at

an identical point.

Page 5: Symmetry in crystals

A unit translation along any axis will

arrive at an identical point

Page 6: Symmetry in crystals

The composition of each unit should

be identical.

Page 7: Symmetry in crystals

A unit translation parallel to any axis will

arrive at an identical point

Page 8: Symmetry in crystals
Page 9: Symmetry in crystals
Page 10: Symmetry in crystals

Face centered lattice

Page 11: Symmetry in crystals
Page 12: Symmetry in crystals

Unit Cell

Page 13: Symmetry in crystals

3 axes, a, b, c and 3 angles , , and

Page 14: Symmetry in crystals
Page 15: Symmetry in crystals
Page 16: Symmetry in crystals
Page 17: Symmetry in crystals
Page 18: Symmetry in crystals

4 3-fold axes along diagonals

Page 19: Symmetry in crystals
Page 20: Symmetry in crystals

4-fold axis

Page 21: Symmetry in crystals
Page 22: Symmetry in crystals

3 2-fold axes

Page 23: Symmetry in crystals
Page 24: Symmetry in crystals

1 6-fold axis

6-fold

Page 25: Symmetry in crystals
Page 26: Symmetry in crystals

A cube with 1 diagonal shortened or lengthened.

Page 27: Symmetry in crystals

3-fold axis

Page 28: Symmetry in crystals
Page 29: Symmetry in crystals

1 2-fold axis

2-fold

Page 30: Symmetry in crystals

2-fold axis

Page 31: Symmetry in crystals

2-fold axis3-fold axis4-fold axis6-fold axis

Page 32: Symmetry in crystals
Page 33: Symmetry in crystals
Page 34: Symmetry in crystals
Page 35: Symmetry in crystals
Page 36: Symmetry in crystals

Symmetry in Crystals

Page 37: Symmetry in crystals

Rotational symmetry

Page 38: Symmetry in crystals

Rotational symmetry

Possible: 2, 3, 4, 6 - fold axes

Page 39: Symmetry in crystals

Rotational inversion

Page 40: Symmetry in crystals

Mirror plane

Page 41: Symmetry in crystals

Screw axes:

a combination

of rotation and

translation.

Page 42: Symmetry in crystals

Screw axes:

a combination

of rotation and

translation.

21 screw = 180o rotation + 1/2 cell translation

Page 43: Symmetry in crystals

31 screw =

120o rotation +

1/3 unit translation

Page 44: Symmetry in crystals
Page 45: Symmetry in crystals

Glide plane:

a combination

of mirror and

translational

symmetry.

Page 46: Symmetry in crystals

Glide plane:

a combination

of mirror and

translational

symmetry.

1/2 unit translation

Page 47: Symmetry in crystals

Given the 7 crystal systems

and various symmetry operations,

the number of ways a continuously

repeating lattice can be formed is

limited.

Page 48: Symmetry in crystals

Theoretical studies of the

geometries of crystals

completed in 1890 demonstrated

that there are 230 ways to put

together an infinitely repeating

lattice.

Page 49: Symmetry in crystals

Unit Cell

Page 50: Symmetry in crystals

Unit Cell

Space group P1

Page 51: Symmetry in crystals

Unit Cell

P1 = primitive cell + inversion center

Page 52: Symmetry in crystals

Unit Cell

P1 = primitive cell + inversion center

Page 53: Symmetry in crystals

Unit Cell

x, y, z = 0, 0, 0

Page 54: Symmetry in crystals

Unit Cell

x, y, z = 1, 0, 0

Page 55: Symmetry in crystals

Unit Cell

x, y, z = 0, 1, 0

Page 56: Symmetry in crystals

Unit Cell

x, y, z = 0, 0, 1

Page 57: Symmetry in crystals

Unit Cell

x, y, z = 1, 0, 1

Page 58: Symmetry in crystals

Unit Cell

x, y, z = 1, 1, 1

Page 59: Symmetry in crystals

Unit Cell

P1 = primitive cell + inversion center

Page 60: Symmetry in crystals

Inversion Center

Cartesian Coordinates:

x, y, z 0, 0, 0

-x, -y, -z -0, -0, -0

Fractional coordinates: the fraction onemust move along each axis to arrive at a point.

Page 61: Symmetry in crystals

Inversion Center

Cartesian Coordinates:

x, y, z 0, 0, 0 1, 0, 0

-x, -y, -z -0, -0, -0 -1, -0, -0

Page 62: Symmetry in crystals

Inversion Center

Cartesian Coordinates:

x, y, z 0, 0, 0 1, 0, 0

-x, -y, -z -0, -0, -0 -1, -0, -0

An integral number of unit translations results in an identical point in the lattice.

Page 63: Symmetry in crystals

Unit Cell

P1 = primitive cell + inversion center

1/2, 1/2, 1/2

Page 64: Symmetry in crystals

Inversion Center

Cartesian Coordinates:

x, y, z 0, 0, 0 1/2, 1/2, 1/2

-x, -y, -z -0, -0, -0 -1/2, -1/2, -1/2

An integral number of unit translations results in an identical point in the lattice.

Page 65: Symmetry in crystals

Unit Cell

P1 = primitive cell + inversion center

1, 1, 1/2

Page 66: Symmetry in crystals

Inversion Center

Cartesian Coordinates:

x, y, z 0, 0, 0 1, 1, 1/2

-x, -y, -z -0, -0, -0 -1, -1, -1/2

An integral number of unit translations results in an identical point in the lattice.

Page 67: Symmetry in crystals

What causes crystals to

form and take a particular structure?

Page 68: Symmetry in crystals

Strong Forces:

Electrostatic forces in ionic crystals.

Page 69: Symmetry in crystals

NaCl

Page 70: Symmetry in crystals

NaCl+ -

Page 71: Symmetry in crystals

NaCl+ -

+ +

+ +

++

- -

--

- -

Page 72: Symmetry in crystals
Page 73: Symmetry in crystals
Page 74: Symmetry in crystals

NaCl ionic bond energy

is 785 kj/mol.

Page 75: Symmetry in crystals

NaCl CsCl

Page 76: Symmetry in crystals

NaCl CsCl

Na+ 1.00 Å Cl- 1.81 Å Cs+ 1.69 Å

Page 77: Symmetry in crystals

NaCl CsCl

Two different cells; same charges;

same stoichiometry.

Page 78: Symmetry in crystals

Determining the contents of

the unit cell.

Page 79: Symmetry in crystals

NaCl

Ion within cell = 1 per cell

Page 80: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell

Ion within cell = 1 per cell

(shared with 2 cells)

Page 81: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion within cell = 1 per cell

(shared with 4 cells)

Page 82: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

Ion within cell = 1 per cell

(shared with 8 cells)

Page 83: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell 0 6

Ion on edge of cell = 1/4 per cell 12 0

Ion at corner of cell = 1/8 per cell 0 8

Na+ Cl-

1 0Ion within cell = 1 per cell

Page 84: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell 0 6

Ion on edge of cell = 1/4 per cell 12 0

Ion at corner of cell = 1/8 per cell 0 8

Na+ Cl-

1 0

Total ions in cell: Na+ Cl-

1 3

Ion within cell = 1 per cell

Page 85: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell 0 6

Ion on edge of cell = 1/4 per cell 12 0

Ion at corner of cell = 1/8 per cell 0 8

Na+ Cl-

1 0

Total ions in cell: Na+ Cl-

1 3 3 1

Ion within cell = 1 per cell

Page 86: Symmetry in crystals

NaCl

Ion on face of cell = 1/2 per cell 0 6

Ion on edge of cell = 1/4 per cell 12 0

Ion at corner of cell = 1/8 per cell 0 8

Na+ Cl-

1 0

Total ions in cell: Na+ Cl-

1 3 3 1

Z = 4

Ion within cell = 1 per cell

Page 87: Symmetry in crystals

Determining ionic radii using

crystal structures.

Page 88: Symmetry in crystals
Page 89: Symmetry in crystals
Page 90: Symmetry in crystals

CsCl

Page 91: Symmetry in crystals

CsCl

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

Ion within cell = 1 per cell

Page 92: Symmetry in crystals

CsCl

Ion on face of cell = 1/2 per cell 0 0

Ion on edge of cell = 1/4 per cell 0 0

Ion at corner of cell = 1/8 per cell 0 8

1 0

Cs+ Cl-

Ion within cell = 1 per cell

Page 93: Symmetry in crystals

CsCl

Ion on face of cell = 1/2 per cell 0 0

Ion on edge of cell = 1/4 per cell 0 0

Ion at corner of cell = 1/8 per cell 0 8

1 0

Cs+ Cl-

Z = 1

Ion within cell = 1 per cell

Page 94: Symmetry in crystals

Ionic crystals are held together

by strong electrostatic forces.

The crystal unit cell is influenced

by ionic sizes.

Page 95: Symmetry in crystals

CaCl2

Page 96: Symmetry in crystals

Ion within cell = 1 per cell

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

CaCl2

Page 97: Symmetry in crystals

Ion within cell = 1 per cell

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

CaCl2

Page 98: Symmetry in crystals

Ion within cell = 1 per cell

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

CaCl2

Page 99: Symmetry in crystals

Ion within cell = 1 per cell

Ion on face of cell = 1/2 per cell

Ion on edge of cell = 1/4 per cell

Ion at corner of cell = 1/8 per cell

CaCl2

Page 100: Symmetry in crystals

Ion within cell = 1 per cell 1 2

Ion on face of cell = 1/2 per cell 0 4

Ion on edge of cell = 1/4 per cell 0 0

Ion at corner of cell = 1/8 per cell 8 0

CaCl2

Ca2+ Cl-

Page 101: Symmetry in crystals

Ion within cell = 1 per cell 1 2

Ion on face of cell = 1/2 per cell 0 4

Ion on edge of cell = 1/4 per cell 0 0

Ion at corner of cell = 1/8 per cell 8 0

CaCl2

Ca2+ Cl-

Z = 2

Page 102: Symmetry in crystals

Diamond

Page 103: Symmetry in crystals

The strengths of chemical bonds: kJ/mol Weak < 200

Average <500>

Strong >800

Page 104: Symmetry in crystals

Diamond

C - C covalent bond = 1.544 Å

Bond enthalpy 348 kJ/mol

Page 105: Symmetry in crystals

Diamond

C - C covalent bond = 1.544 Å

Bond enthalpy 348 kJ/mol

Page 106: Symmetry in crystals

Diamond

Atom within cell = 1 per cell

Atom on face of cell = 1/2 per cell

Atom on edge of cell = 1/4 per cell

Atom at corner of cell = 1/8 per cell

Page 107: Symmetry in crystals

Diamond

Atom within cell = 1 per cell 4

Atom on face of cell = 1/2 per cell

Atom on edge of cell = 1/4 per cell

Atom at corner of cell = 1/8 per cell

C

Page 108: Symmetry in crystals

Diamond

Atom within cell = 1 per cell 4

Atom on face of cell = 1/2 per cell 6

Atom on edge of cell = 1/4 per cell

Atom at corner of cell = 1/8 per cell

C

Page 109: Symmetry in crystals

Diamond

Atom within cell = 1 per cell 4

Atom on face of cell = 1/2 per cell 6

Atom on edge of cell = 1/4 per cell 0

Atom at corner of cell = 1/8 per cell

C

Page 110: Symmetry in crystals

Diamond

Atom within cell = 1 per cell 4

Atom on face of cell = 1/2 per cell 6

Atom on edge of cell = 1/4 per cell 0

Atom at corner of cell = 1/8 per cell 8

C

Page 111: Symmetry in crystals

Diamond

Atom within cell = 1 per cell 4

Atom on face of cell = 1/2 per cell 6

Atom on edge of cell = 1/4 per cell 0

Atom at corner of cell = 1/8 per cell 8

C

Z = 8

Page 112: Symmetry in crystals

Molecular Crystals

Page 113: Symmetry in crystals

Molecular Crystals:

Consist of repeating arrays

of molecules and/or ions.

Page 114: Symmetry in crystals
Page 115: Symmetry in crystals
Page 116: Symmetry in crystals

C17H24NO2+ Cl- . 3 H2O

Page 117: Symmetry in crystals

V = 974.45 Å3

C17H24NO2+ Cl- . 3 H2O FW = 363.87 g/mol

Z = 2

Density =727.74 g

5866.19 x 10-1cm3

Density =363.87 g (2)

974.45 x 10-24 x 6.02 x 1023

= 1.241 g/cm3

Page 118: Symmetry in crystals

C17H24NO2+ Cl- . 3 H2O

Page 119: Symmetry in crystals
Page 120: Symmetry in crystals

Although Z = 2, the unit cell containsportions of a number of molecules.

Page 121: Symmetry in crystals

Cl-

Page 122: Symmetry in crystals

Cl-

Page 123: Symmetry in crystals

Cl-

H2O

Page 124: Symmetry in crystals

Cl-

H2O

Hydrogen bondsCl OH2

Page 125: Symmetry in crystals
Page 126: Symmetry in crystals

Hydrogen bond

Page 127: Symmetry in crystals
Page 128: Symmetry in crystals

Model with atoms having VDW radii.

Page 129: Symmetry in crystals
Page 130: Symmetry in crystals

C17H24NO2+ Cl- . 3 H2O

Although this material is ionic, the + and - chargesare not close enough tocontribute to the formationof the crystal.

Page 131: Symmetry in crystals

Molecular crystals tend to be

held together by forces weaker than

chemical bonds.

van der Waal’s forces are always

a factor.

Hydrogen bonding is often present.

Page 132: Symmetry in crystals
Page 133: Symmetry in crystals

A layer in an ionic solid with ionsof similar radii.

Page 134: Symmetry in crystals
Page 135: Symmetry in crystals
Page 136: Symmetry in crystals
Page 137: Symmetry in crystals