P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
http://folk.uio.no/ravi/CMP2015
Prof.P. Ravindran, Department of Physics, Central University of Tamil
Nadu, India
Atomic packing in solids
1
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Periodic table of
elements
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Periodic table
of elements
3
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
4
Electronegativity Review
Electronegativity: A measure of the attractive force that one atom in a covalent bond has for the electrons of the bond
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
(Primitive cubic)
Crystal Structure of Metals5
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Calculation of an octahedral interstitial site
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Closest Packing
Holes
7
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 8
Packing Of Spherical Vegetables
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Atomic packing in Metals
Closest Packing:
Assumes that metal atoms are uniform, hard
spheres.
Spheres are packed in layers. Like oranges in
grocery store display
abab packing - 3rd directly over 1st layer - called
hexagonal closest pack (hcp)
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Atomic packing in Metals (con’t)
abca packing - 3rd layer not directly over 1st, 4th layer is
over 1st - cubic closest pack (ccp) or face centered cubic
(fcc) see next slide
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Face Centered Cubic (FCC)
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Metallic Bonding Nearest Neighbors
The Indicated Sphere Has 12 Nearest Neighbors
Each sphere in closest packed
(both fcp and hcp) has 12
equivalent nearest neighbors.
12
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Unit cell atoms
fcc and hcp
8 x 1/8 spheres and 6 x 1/2
spheres = 4 total atoms in
unit cell
13
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Close-Packing of Spheres
Many solids have close-packed structures in which spherical
particles are arranged in order to leave the minimum amount of
space.
There are two forms of close-packing; cubic close-packing and
hexagonal close-packing.
In both cases, each sphere has a coordination number of 12,
which means the each sphere has 12 equidistant neighbors.
There are 6 neighbors in one plane, 3 below and 3 above.
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Hexagonal
close- packing
Cubic close-
packing
Hexagonal and cubic close packing15
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Hexagonal Closest Packing
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Cubic Closest Packing
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The abab staching in
hcp lattice.
The Indicated Sphere Has 12
Nearest Neighbors
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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Packing in Metals
Model: Packing uniform, hard spheres to best use available
space. This is called closest packing. Each atom has 12
nearest neighbors.
hexagonal closest packed (“hcp”)
cubic closest packed (“ccp”)
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Co-ordination number
•Number of spheres which are
touching a particle sphere
•In ionic crystals Number of oppositely charged
ions surrounding a particular ion
e.g., Co-ordination number of
Cl– and Na+ in NaCl molecule is 6
each.
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Simple cubic
How do we count nearest neighbors?
Coordination Number
Draw a few more unit cells…...
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 22
Simple cubic
Highlight the nearest neighbors….
Coordination Number
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
coordination number of 6
What about body centered cubic?????
Simple Cubic
COORDINATION NUMBER
How many nearest neighbors???
23
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
24
In the three types of cubic unit cells:
Simple cubic
Coordination Number
CN = 6
Body Centered cubic CN = ?
Lets look at this…….
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
25
In bcc lattices, each sphere has a coordination number of 8
Body-centered cubic packing (bcc)
COORDINATION NUMBER?????
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
26
The Position of Tetrahedral Holes in a Face-
Centered Cubic Unit Cell
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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Cubic Closest
Packing in NaCl
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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The Net Number of Spheres in a Face-
Centered Cubic Unit Cell
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Alloys
An alloy is a blend of a host metal and one or more
other elements which are added to change the
properties of the host metal.
Ores are naturally occurring compounds or
mixtures of compounds from which elements can be
extracted.
Bronze, first used about 5500 years ago, is an
example of a substitutional alloy, where tin atoms
replace some of the copper atoms in the cubic array.
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Metal Alloys
Substitutional Alloy:
some metal atoms
replaced by others of
similar size.
brass = Cu/Zn
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Metal Alloys(continued)
Interstitial Alloy:
Interstices (holes) in closest
packed metal structure are
occupied by small atoms.
steel = iron + carbon
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Bronze
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Substitutional Alloy
Examples
Where a lattice atom is replaced by an atom of
similar size
• Brass, one third of copper atoms are replaced by
zinc atoms
• Sterling silver (93% Silver and 7%Cu)
• Pewter (85% Sn, 7% Cu, 6% Bi, and 2% Sb)
• Plumber’s solder (67% Pb and 33% Sn)
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Alloys
– Interstitial Alloy
When lattice holes (interstices) are filled with smaller atoms
Steel best known interstitial alloy, contains carbon atoms in the holes of an iron crystal
– Carbon atoms change properties
Carbon a very good covalent bonding atom changes the non-directional bonding of the iron, to have some direction
Results in increased strength, harder, and less ductile
The larger the percent of carbon the harder and stronger the steel
Other metals can be used in addition to carbon, thus forming alloy steels
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Carbon Steel
Unlike bronze the carbon atoms fit into the holes formed by
the stacking of the iron atoms. Alloys formed by using the
holes are called interstital alloys.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 10–36
Two Types of
Alloys
Substitutional
Interstitial
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 37
The fraction of the volume that is actually occupied by spheres…..
cellunit the of volume
cellunit the in spheres the by occupied volumevf
Efficiency Of Packing
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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Fraction(f) Of The Volume Occupied By The Spheres In The Unit
Cell.
unitcell
spheresv
V
Vf
Vspheres= number of spheres x volume single sphere
Vunit cell = a3 cubic unit cell of edge length a
Lets get NUMBER OF SPHERES
cellunit the of volume
cellunit the in spheres the by occupied volumevf
Packing Efficiency
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 39
Packing Efficiency
•Counting atoms in a unit cell!
•Atoms can be wholly in a unit
cell or atoms shared
between adjacent unit cells
In the lattice Counts 1 for atom in cell
Counts for 1/2 atom on a face.
Counts for 1/4 atom on a face.
Counts as 1/8 for atom on a corner.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
40
What is the number of spheres in the fcc unit cell?
Total spheres = 8 (1/8) + 6 (1/2)
= 1 + 3 = 4
Face-centred Cubic Unit Cell
Note: 1/8 of a sphere on 8 corners and ½ of aSphere on 6 faces of the cube
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing Spheres into Lattices
The most efficient way to pack hard spheres is
Spheres are packed in layers in which each sphere is surrounded by
six others.
CLOSEST PACKING
First Layer
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing Spheres into Lattices:
Next Layer The next spheres fit into
a “dimple” formed by three spheres in the first layer.
There are two sets of dimples…...
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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Packing Spheres into Lattices:
Next Layer The next spheres fit into
The two types of “dimples” formed by three spheres in the
first layer.The second layer…..
NOTE: the
inverted
triangleTriangle
not
inverted
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Tetrahedral site Octahedral site
Closed packed structure44
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 45
Packing Spheres into Lattices:
Second Layer
Once one is put on the others are forced into half of the dimples of the same type….
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 46
Packing Spheres into Lattices
Once one is put on the others are forced into half of the dimples of the same type….
Second Layer
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 47
Packing Spheres into Lattices
Second Layer
Note that the second layer only occupies half the dimples in the first layer.
Inverted triangle dimples are
not filled.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing Spheres into LatticesSecond Layer
Note that the second layer only occupies half the dimples in the
first layer.
Occupied
dimple
Unoccupied
DIMPLE
THE THIRD LAYER…...
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 49
Packing Spheres Into Lattices
The aba arrangement of layers, option 1.
A
B
A
HEXAGONAL CLOSEST PACKING
A HEXAGONAL UNIT CELL.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 50
HCP
Hexagonal Unit Cell
ABA ARRANGEMENT HAS A HEXAGONAL UNIT CELL.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 51
SUMMARY
NOW OPTION TWO…..
EXPANDED VIEW
HEXAGONAL CLOSED PACKED STRUCTURE
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 52
1
11
Packing Spheres Into Lattices
(1) a dimple directly above sphere in the first layer
THIRD LAYER, Choose a dimple
NOTE: the inverted triangle
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
OPTION 2!
THIS DIMPLE DOES NOT
2 2
2
LIE DIRECTLY OVER THE SPHERES OF THE FIRST LAYER.
Packing Spheres Into Lattices
THIRD LAYER
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 54
GREEN SPHERES DO NOT LIE DIRECTLY OVER THE SPHERES OF THE FIRST LAYER.
THE THIRD LAYER IS DIFFERENT FROM THE FIRST…….
Packing Spheres Into Lattices
THIRD LAYER
OPTION 2
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 55
A
B
C
NOT THE SAME AS OPTION ONE!
WE CALL THE THIRD LAYER C THIS TIME!
Packing Spheres Into Lattices
THIRD LAYER OPTION 2
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
A
B
C
The ABC Arrangement of layers.
We call the third layer C this time!
NOW THE FOURTH LAYER…….
OPTION 2
Packing Spheres Into Lattices
Third Layer
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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A
B
C
Fourth Layer The Same As First.
Packing Spheres Into Lattices
FOURTH LAYER
PUT SPHERE IN SO THAT
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
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A
B
C
The ABCA Arrangement………..
Fourth Layer The Same As First.
Packing Spheres Into Lattices
A
This Is Called Cubic Closed Packed
….
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 59
Unit Cell Of CCP
Face- Centred Cubic Unit Cell (FCC)
This ABCA arrangement has a
A Comparison…..
CUBIC UNIT CELLL
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
COMPARISON
HCP CCPNOTICE the flip…...
NEAREST NEIGHBORS…..
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing in Ionic Crystals
Ions pack themselves to maximize the attractions and
minimize repulsions between the ions.
AAA pack = primitive unit, coordination# 8
ABA packing = body-centered unit, coordination# 12
ABCA packing = face-centered unit, coordination# 12
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Structures of Metals
Closest Packing
1. Hexagonal
2. Cubic
A-B A-B-C
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 63
COORDINATION NUMBER
The number of nearest neighbors that a lattice point has in a
crystalline solid
Lets look at hcp and ccp…...
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 64
HCP CCP
Coordination Number =12
Coordination Number
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Spaces In Ionic Solids Are Filled With
Counter Ions
In NaCl, the Cl- ions form a
unit cell that is face centered
cubic
Na+ ions, being smaller, fill
the spaces between the Cl-
ions
If we count the atoms in the
unit cell we have 6 of each,
thus a 1:1 Na+:Cl- ratio
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The three cubic unit cells.
Simple Cubic
coordination number = 6
Atoms/unit cell = 1/8 * 8 = 1
1/8 atom
at 8
corners
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The three cubic unit cells.
Body-centered
Cubic
coordination number = 8
1/8 atom
at 8
corners1 atom at
center
Atoms/unit cell = (1/8*8) + 1 = 2
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The three cubic unit cells.
Face-centered
Cubic
coordination number = 12
Atoms/unit cell =
(1/8*8)+(1/2*6) = 4
1/8 atom
at 8
corners
1/2 atom
at 6 faces
68
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
End centered cubic unit cell
Total no. of constituents per unit cell.
= Total contribution by constituents at corners
+ Total contribution by particles on the faces.
=8 x 1/8 + 1/2 x 2
=1 + 1
=2
69
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Hexagonal close packed
structure
Consists of atoms with ABABAB stacking.
Each atom is surrounded by 12 closest neighbors.
Packing efficiency is 74%.
70
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Cubic close packed structure
Consists of atoms with ABCABCABC stacking.
Each atom is surrounded by 12 closest neighbours.
Packing efficiency is 74%.
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing Structures
• Both structures have coordination number of 12
o 74% of total volume of structure is occupied by spheres
o 26% empty space between spheres
• When unequal-sized spheres are packed into lattice
o Large particles usually assume one of the close packing
arrangements
o Small particles fill the holes between larger particles
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Fraction of an Atom that Occupies a Unit Cell
for Various Positions in the Unit Cell
Positions in Unit Cell Fraction in Unit Cell
Center 1
Face ½
Edge ¼
Corner 1/8
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Calculating Mass of Atoms
Make sure you know the volume or solve for it
Know the atoms per unit cell (given)
Know the density of atom (given)
Solve for mass using d =m / V
This gives you mass per unit cell and multiple by atoms per
unit cell
74
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Cubic unit
cells
The unit cell forms the basic repeating unit of a crystal lattice.
The cubic unit cell is the simplest type.
75
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Coordination Numbers
Coordination # Percent of molecule occupied
Single Cubic 6 52%
Face 12 74%
Body 8 68%
Hexagonal 12 74%
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Geometry of a Cube
2
Diagonal Face
222
ef
eef
3
3
DiagonalBody
2222
eb
efeb
77
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Atomic Radius and Cell Dimensions
Simple Cubic
r = e/2
1 atom/unit cell (in metals)
Body-Centered Cubic
b = 4r = e(3)1/2
r = e(3)1/2/4
2 atoms/unit cell (in metals)
Face-Centered Cubic
f = 4r = e(2)1/2
r = e(2)1/2/4
4 atoms/unit cell (in metals)
78
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
• Tend to be densely packed:
Metallic Crystal Structures
vs.
FCC and HCP close-packed BCC not close-packed
- Minimize empty space
79
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids 80
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
1H He
1 2
2Li Be B C N O F Ne
2,1 2,2 2,3 2,4 2,5 2,6 2,7 2,8
3Na Mg Al Si P S Cl Ar
2,8,1 2,8,2 2,8,3 2,8,4 2,8,5 2,8,6 2,8,7 2,8,8
4K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
2,8,8,1 2,8,8,2 2,8,9,22,8,10,
22,8,11,
22,8,13,
12,8,13,
22,8,14,
22,8,15,
22,8,16,
22,8,18,
12,8,18,
22,8,18,
32,8,18,
42,8,18,
52,8,18,
62,8,18,
72,8,18,
8
5Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
2,8,188,1
2,8,188,2
2,8,189,2
2,8,1810,2
2,8,1812,1
2,8,1813,1
2,8,1814,1
2,8,1815,1
2,8,1816,1
2,8,1818,0
2,8,1818,1
2,8,1818,2
2,8,1818,3
2,8,1818,4
2,8,1818,5
2,8,1818,6
2,8,1818,7
2,8,1818,8
6
Cs Ba * Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
2,8,1818,8,1
2,8,1818,8,2
2,8,1832,10,2
2,8,1832,11,2
2,8,1832,12,2
2,8,1832,13,2
2,8,1832,14,2
2,8,1832,15,2
2,8,1832,17,1
2,8,1832,18,1
2,8,1832,18,2
2,8,1832,18,3
2,8,1832,18,4
2,8,1832,18,5
2,8,1832,18,6
2,8,1832,18,7
2,8,1832,18,8
Fr Ra ** Rf Db Sg Bh Hs Mt Uun Uuu Uub
2,8,18,3218,8,1
2,8,18,32
18,8,2
2,8,18,32
32,10,2
2,8,18,32
32,11,2
2,8,18,32
32,12,2
2,8,18,32
32,13,2
2,8,18,32
32,14,2
2,8,18,32
32,15,2
2,8,18,32
32,17,1
2,8,18,32
32,18,1
2,8,18,32
32,18,2
Element Groups (Families)
Alkali Earth Alkaline Earth Transition Metals
Rare Earth Other Metals Metalloids
Non-Metals Halogens Noble Gases
http://www.chemicalelements.com/show/electronconfig.html
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing fraction
• Packing fraction is the fraction of total volume of a
cube occupied by constituent particles.
Packing fraction(PF) =
Volume occupied by effective number of particles
Volume of the unit cell
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing of spheres in the unitcell.
simple cubic
(52% packing
efficiency)
body-centered
cubic
(68% packing
efficiency)
83
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
hexagonal
unit cell
closest packing of
first and second
layers
layer a
layer a
layer b
layer c
hexagonal
closest
packing cubic closest
packing
abab… (74%)
abcabc… (74%)
face-centered
unit cell
84
Packing of spheres in the unitcell.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing fraction of simple cubic crystal
For simple cubic crystal(scc)
Packing fraction =
3
3
41 r
3
a
3
3
4r
3 a 2r 0.5232r
For bcc, body diagonal, 4r 3a
Packing fraction =
3
3
42 r
3 0.68 i.e., 68%
4r
3
aA B
85
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Packing fraction of face cubic crystal
For fcc, face diagonal, 4r = 2a
Packing fraction =
3
3
44 r
3 0.74 i.e., 74%
4r
2
A B
C
a
86
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Calculating the Packing Factor
74.018)2/4(
)3
4(4)(
Factor Packing
24r/ cells,unit FCCfor Since,
)3
4)(atoms/cell (4
Factor Packing
3
3
0
3
0
3
r
r
r
a
a
Calculate the packing factor for the FCC cell.
SOLUTION
In a FCC cell, there are four lattice points per cell; if there is one atom
per lattice point, there are also four atoms per cell. The volume of one
atom is 4πr3/3 and the volume of the unit cell is . 3
0a
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Density
The number of particles present per unit cell.
Suppose the edge length of the unit cell = a
Number of atoms present in one unit cell = Z
Atomic mass of the element = M
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P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Density
Density of unit cell (r) =Mass contained in one unit cell
Volume of the unit cell
Mass contained in one unit cell =
Number of particles in one unit cell × Mass of one particle
Since mass of one particle = Atomic mass
Avogadro ' s number
89
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
• Coordination # increases with
Coordination # and Ionic Radii
ZnS
(zincblende)
NaCl(sodium
chloride)
CsCl(cesium chloride)
rcation
ranion
Issue: How many anions can you
arrange around a cation?
2
rcationranion
Coordination
Number
< 0.155
0.155 - 0.225
0.225 - 0.414
0.414 - 0.732
0.732 - 1.0
3
4
6
8
linear
triangular
Tetrahedron
Octahedron
cubic
Coordination
Geometry
(Cation-anion radius ratio)
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Cation Site Size
Determine minimum rcation/ranion for OH site (C.N. = 6)
a 2ranion
2ranion 2rcation 2 2ranion
ranion rcation 2ranion
rcation ( 2 1)ranion
2ranion 2rcation 2a
4140anion
cation .r
r
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
This is the NaCl structure.
Two interpenetrating fcc arrays, one of Na+ ions and one
of Cl- ions.
The Na+ sit in the holes of the black (Cl-) lattice
SO HOW WE DESCRIBE IONIC SOLIDS???
Cl-
Na+
NaCl structure93
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The anion is usually larger than the cation.
We describe an ionic solid as a lattice of the larger ions with the
smaller ions occupying holes in the lattice.
Consist of two interpenetrating lattices of the
two ions (cations and anions) in the solid.
NOTE:
Ionic Solids
HOLES????
94
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The yellow dots form a FCC lattice!
Holes In A FCC Lattice
95
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The yellow dots form a fcc lattice!
HOW MANY HOLES??????
Holes In A FCC Lattice96
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Holes In a FCC Lattice
The holes:
THIRTEEN: ONE IN THE CENTRE
How many??
12 on the edges.
What shape is the hole ?
97
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
98
OCTAHEDRAL HOLES:
There is one octahedral hole in the centre of the unit cell.
Central Hole
If each one is occupied by an atom?
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
There are 4 complete octahedral holes per fcc unit cell.
The Octahedral Holes
If each one is occupied by an atom?
How many atoms per unit cell?
Number of atoms = 1 + 12 x (1/4) = 4
1/4 atom1 atom
Notice that the number of octahedral holes is the same as the number of atoms forming the unit cell!!
99
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The Octahedral Holes
Other holes…..
Between two layers…..
10
0
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
There are other holes!
Where are the other holes in the FCC unit cell?
Can you spot them??????
Look at one of the small cubes
Other Holes10
1
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Small Cube
Take a point at the centre of this cube
There are eight of these….
10
2
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
There is one tetrahedral hole in each of the eight smaller cubes in
the unit cell.
All the holes are completely within the cell, so there are 8 tetrahedral
holes per fcc unit cell
Notice that there are twice as many tetrahedral holes as atoms forming the lattice! That would be 8 holes.
Tetrahedral Holes10
3
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Tetrahedral Holes
Formed by three spheres in one layer and
There is one more hole……….
one sphere in another layer sitting in the dimple they form.
104
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Formed from the space between three ions in a plane.
Trigonal Holes
Formed by three spheres in one layer.
The smallest hole!
105
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Atomic Size Ratios and the Location of Atoms in Unit Cells
Packing Type of Hole Radius Ratio
hcp or ccp Tetrahedral 0.22 - 0.41
hcp or ccp Octahedral 0.41 - 0.73
Simple Cubic Cubic 0.73 - 1.00
About Holes in Cubic Arrays
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
M+ or M2+ cations always occupy the holes
Consequently the radius of the cation must be
This causes the X– anions to be pushed apart,
greater than the size of the hole!
which reduces the X– – X– repulsion.
with the largest coordination number without rattling around!
Which hole will a cation occupy??????
Tight Fit
So we will investigate the size of these holes!
They occupy the holes that result in maximum attraction and minimum repulsion.
108
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Investigate the size of these holes!
Which hole will a cation occupy??????
The size of the hole depends upon the
size of the ion (usually anion) that forms the lattice into which
the cations are to go……...
OCTAHEDRAL HOLE IN FCC….
109
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Look at plane
Draw a square.
Put in spheres.
Fit a small sphere in
This will be the cation
These are the anions
Draw diagonal
Put in distances……..
Octahedral Holes In FCC 110
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
R
R
R
R
2r
Radius of ion = R
Look at plane
Radius of hole = r+(2R)2(2R)2 = (2R + 2r)2
8R2 = (2R + 2r)2
rRR 2222
rR 2)222(
rR 12
0.414R = r
Octahedral Holes In FCC111
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
R
R
R
R
2r
Radius of anion = R
Look at plane
Radius of hole = r
0.414R = r
The size of cation that just fits has a
radius that is
0.414 x radius of anion(R)
roctahedral hole = 0.414 R
What about the tetrahedral hole?
Octahedral Holes In FCC112
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Using similar calculations, we can find the radius of other types
of holes as well:
rtetrahedral = 0.225 R
r = radius of ion fitting into hole (usually the cation)
The ratio between the radius of a hole in a cubic lattice
R is the radius of the ion forming the lattice (usually the anion).
fcc
RADIUS RATIO:
and the radius of the ions forming the hole
roctahedral = 0.414 R
What about other cubic cell systems??
DO IT!!!!!!!
113
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
rcubic = 0.732 Ranion
If the M+ cations (e.g. Cs+) are sufficiently large,
The next best closest packed X– array adopted by the anions is
a simple cubic structure, giving cubic holes which are large
enough to hold the cations.
Simple Cubic
they can no longer fit into octahedral holes of a fcc lattice.
YOU can show that...
114
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The cubic hole
The coordination number in the cubic hole is ?
The coordination number in the
fcc tetrahedral hole is ?
4!
The coordination number in the
fcc octahedral hole is ?
6!
8
In contrast for a fcc lattice…...
rcubic = 0.732 Ranion
115
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Summary:
Face centred cubic:
Trigonal hole Too small to be occupied
Tetrahedral hole CN = 4 rcation = 0.225Ranion
Octahedral hole CN = 6
8 of these
rcation = 0.414Ranion 4 of these
Simple cubic:
Cubic hole CN = 8 rcation = 0.732Ranion 1 of these
For a given anion
rtrigonal < rtetrahedral < roctahedral < rcubic
116
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Into Which Hole Will The Ion Go??
TETRAHEDRAL
The hole filled is tetrahedral if:
0.225Ranion < rcation < 0.414Ranion
rtetrahedral < rcation < roctahedral
117
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Into Which Hole Will The Ion Go??
OCTAHEDRAL
The hole filled is octahedral if:
0.414Ranion < rcation < 0.732Ranion
roctahedral < rcation < rcubic
118
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Into Which Hole Will The Ion Go??
CUBIC
The hole filled is cubic if:
0.732Ranion < rcation
Lets look at these ideas in action…….
rcubic < rcation
119
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Na+
has a radius of 98pm.Cl
-has a radius of 181pm.
Consider a fcc array of Cl- then:
Radius of the tetrahedral hole is 0.225 x 181=41pm
Radius of the octahedral hole is 0.414 x 181=75pm
Consider a sc array of Cl- then:
Radius of the cubic hole is 0.732 x 181=132pm
So the best fit is the octahedral hole in the fcc array!
The 98pm is bigger than 75pm but less than 132!
OR USING RATIOS…….
NaCl120
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Na+
has a radius of 98pm.Cl
-has a radius of 181pm.
54.0181
98
pm
pm
r
r
r
r
Cl
Na
anion
cation
225.0tet
anion
tet
cation
r
r414.0
oct
anion
oct
cation
r
r732.0
cubic
anion
cubic
cation
r
r
0.54 lies between 0.414 and 0.732
so the sodium cations will occupy octahedral holes
in a fcc (ccp) lattice
NaCl121
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
1:1 stoichiometry is required
How many complete octahedral holes in face centred cubic array
of Cl- ?????
So stoichiometry is ok!!
4
How many Cl- needed to form the fcc array??? 4
Therefore 4 Cl- and 4 Na+
NaClIs the stoichiometry ok??? 122
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Example: Predict the structure of Li2S
Li+
is 68 pm S2-
is 190pm
36.0190
68
2
pm
pm
r
r
r
r
S
Li
anion
cationCalculate ratio..
Examine the cation-anion radius ratios to find which type of
holes the smaller ions fill
STEP ONE:
225.0tet
anion
tet
cation
r
r414.0
oct
anion
oct
cation
r
r
COMPARE with ratios….
Which is the best hole???? TETRAHEDRAL!!!!
123
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
This requires tetrahedral holes.
Example: Predict the structure of Li2S
Li+ is 68 pm S2- is 190pm
36.0190
68
2
pm
pm
r
r
r
r
S
Li
anion
cation
face- centred cubic array
Lets look at the structure…...
Calculate ratio..
Which lattice has tetrahedral holes???
Thus the S2- will form a fcc lattice ...
124
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
FCC unit cell with tetrahedral holes
ANION
CATION
There are 8 tetrahedral
holes.
How many are occupied?
Four anions in the unit cell.
STEP TWO: Determine what fraction of those holes must be
filled to give the correct chemical formula
125
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
FCC unit cell with tetrahedral holes
S2-
Li+
How many are occupied?
Li2S needs two Li+ for each S2-
Four anions in the
unit cell.
There are 8 tetrahedral
holes.
Therefore all the tetrahedral holes are occupied!
126
Li2S is a face centered lattice of S2- with
all of the tetrahedral holes filled by Li+
ions.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
CsCl: Cs+ is 167 pm Cl- is 181pm Calculate ratio
0.92 is greater than 0.732
92.0181
167
pm
pm
r
r
r
r
Cl
Cs
anion
cation
the cesium cations will occupy cubic holes of a simple cubic lattice.
732.0cubic
anion
cubic
cation
r
rCompare…...
127
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
There are the same number of cubic holes and lattice points in the
cubic lattice.
Hence stoichiometry OK!
CsCl is composed of a simple cubic lattice of chloride anions with
cesium cations in all the cubic holes.
128
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Cesium Chloride129
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
ZnS: Zn2+ is 64 pm S2- is 190 pm Calculate ratio
35.0190
64
2
2
pm
pm
r
r
r
r
S
Zn
anion
cation
225.0tet
anion
tet
cation
r
r414.0
oct
anion
oct
cation
r
rCOMPARE
This requires
tetrahedral holes.
The sulfide ions will form a face-centered cubic array
because….
that is the only type to possess tetrahedral holes.
130
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
We need an equal number of zinc and sulfide ions.
There are the twice as many tetrahedral holes(8) as S2-(4) that
form the fcc lattice.
Therefore, half the
tetrahedral holes will be
filled.
131
ZnS is composed of a fcc lattice of sulfide anions with zinc cations in half the
tetrahedral holes.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
There are two forms of ZnS
This is an example
of polymorphism.
One is the zinc blende that we have talked about!
The other is wurtzite based on hcp lattice.
132
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX- Type Crystal Structure
Ceramic materials which have equal number of cations
and anoins.
AX compounds
– A = cation
– X = anion
Consists of :
– Rock Salt/ Sodium Chloride (NaCl ) structure
– Cesium Chloride Structure
– Zinc Blende Structure
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
• On the basis of ionic radii, what crystal structure
would you predict for FeO?
• Answer:
5500
1400
0770
anion
cation
.
.
.
r
r
based on this ratio,
--coord # = 6
--structure = NaCl
Example 1: Predicting Structure of FeO
Ionic radius (nm)
0.053
0.077
0.069
0.100
0.140
0.181
0.133
Cation
Anion
Al3+
Fe2+
Fe3+
Ca2+
O2-
Cl-
F-
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX- Crystal Structure: Rock Salt Structure
Same concepts can be applied to ionic solids in general.
Example: Sodium Chloride (NaCl ) / rock salt structure
rNa = 0.102 nm
rNa/rCl = 0.564
cations prefer OH sites
rCl = 0.181 nm
The coordination number is 6
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX-Crystal Structure :Rock Salt Structure
MgO and FeO also have the NaCl structure
O2- rO = 0.140 nm
Mg2+ rMg = 0.072 nm
rMg/rO = 0.514
cations prefer OH sites
So each oxygen has 6 neighboring Mg2+
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX-Crystal Structures: Cesium Chloride
Structure
939.0181.0
170.0
Cl
Cs
r
r
Cesium Chloride structure:
cubic sites preferred
So each Cs+ has 8 neighboring Cl-
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX-Crystal Structures: Zinc Blende
So each Zn2+ has 4 neighboring O2-
Zinc Blende structure?? 529.0
140.0
074.0
2
2
O
ZnHO
r
r
• Size arguments predict Zn2+
in OH sites,
• In observed structure Zn2+
in TD sites
Why is Zn2+ in TD sites?
– bonding hybridization of
zinc favors TD sites
Ex: ZnO, ZnS, SiC
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
AX2 Type Crystal Structures
Fluorite structure
• Calcium Fluorite (CaF2)
• cations in cubic sites
• UO2, ThO2, ZrO2, CeO2
• Antifluorite structure –
cations and anions
reversed.
•Charges of cation and anions are
not the same
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
ABX3 Crystal Structures
Ceramic compound have more than one type of cation
Perovskite
Ex: complex oxide
BaTiO3
(Barium Titanate)
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
(c) 2003 Brooks/Cole Publishing / Thomson Learning™
Figure 3.31 Connection between anion polyhedra. Different possible connections include sharing of corners, edges,
or faces. In this figure, examples of connections between tetrahedra are shown.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
The perovskite unit cell showing the A and B site cations and oxygen ions
occupying the face-center positions of the unit cell. Note: Ions are not show to
scale.
P.Ravindran, PHY074- Condensed Matter Physics, Spring 2015 : Atomic packing in solids
Crystal Structure of Ceramic