2. Crystal
A crystal is a homogeneous, anisotropic solid
body having long-range 3D ordering (order may
be Translational/orientational/combination of
both), i.e., constructed by infinite repetition of
identical structural units.
Features:
• Natural shape of polyhedron
• Chemical compound
• Under the action of interatomic forces
• End phase generally becomes solid when passing from
phase transformation under suitable conditions
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3. Lattice
Space-lattice is a mathematical concept, defined
as infinite number of regular periodic arrays of
points in 3D configuration having long-range
ordering (both in translational & orientational),
with the property that arrangement of points
about any particular point is isotropically
identical.
a2
a
3
a1
u2a2
u
3
a
3
1 1 2 2 3 3
r u a u a u a
= + +
where are translational vectors
1 2 3
, ,
a a a
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4. Basis
It is the group of atoms, identical in composition, arrangement and orientation, when
repeated in space periodically and isotropically, forms crystal structure.
Basis Lattice Crystal
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5. Crystalline Solid Amorphous Solid
Atomic
Arrangement
Atoms are arranged in a regular,
repeating pattern
Atoms are arranged randomly,
lacking a long-range order
Melting Point Have a sharp, distinct melting
point
Melt over a range of temperatures,
not a specific point
Hardness When broken, crystalline solids
tend to cleave along specific
planes due to their ordered
structure
Break with irregular or curved
surfaces, not along defined planes
X-ray
Diffraction
Produce sharp, well-defined X-
ray diffraction patterns due to
their ordered structure
Produce broad, diffuse patterns or
no diffraction pattern at all,
indicating the lack of long-range
order
Anisotropy/
Isotropy
Can be anisotropic (physical
properties vary depending on
direction)
Generally isotropic, with similar
properties in all directions
Example Diamond, quartz, salt Glass, rubber, plastic
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6. Unit Cell
Smallest geometric arrangement whose
repetition in 3D space gives actual crystal
structure.
This elementary pattern of minimum number of
points carry all the characteristics of the crystal.
Unit cell Crystal formation
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7. Primitive Cell
It is the unit cell which contains lattice points at
corners only.
It is the minimum volume unit cell, and will fill
all the space by repetition of suitable crystal
translational operations.
Each primitive cell is associated with one lattice
point.
No. of atoms in a primitive cell is always the same
for a given crystal structure.
1 2 3
.
p
V a a a
=
Crystal formation
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8. Primitive Cell Unit Cell
Repeating
pattern
simplest repeating unit in a
crystal structure
larger repeating unit that can be
primitive or non-primitive
No of points Contains only one lattice point,
which is typically located at the
corners of the cell
Non-primitive unit cells (also
called centered unit cells) contain
additional lattice points within the
cell, along with corner point
Example A cubic primitive unit cell has
lattice points only at the corners
BCC unit cell has lattice points at
the corners and one in the center.
FCC unit cell has lattice points at
the corners and in the center of
each face
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9. Bravis Lattice
Network of part where position vectors can be expressed
in the form
1 1 2 2 3 3
r u a u a u a
= + +
where the choice of basis vectors is not unique.
A primitive unit cell is called Bravis lattice.
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10. Classification of Cubic Lattice
Cubic Lattice
Simple Cubic
Body-Centered
Cubic (BCC)
Face-Centered
Cubic (FCC)
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11. A few properties
Coordination number: It is defined as number of equidistant neighbor that an atom has in the
given structure
Packing Fraction: It is defined as the maximum proportion of available volume in a unit cell
that can be occupied by the closed pack spheres
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12. Simple Cubic Lattice
Unit cell contains 8 atoms, 1 in each corner
Each corner atom is shared among 8 cells, so
Total no of atoms per unit cell = 8⨯(1/8)=1
No. of atoms per unit cell = 1
Coordination no. = 6
Distance between any two corner atoms = ‘a’
So, radius of closed-packed sphere r = 0.5a
Atomic radius = 0.5a
Packing fraction =
3
3
4
3
r
a
3
3
4
3.8
a
a
= 0.523
6
= =
P.F = 0.523
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13. Body-Centered Cubic Lattice
Unit cell contains 9 atoms, 1 in each corner
and 1 in center
Each corner atom is shared among 8 cells, so
Total no of atoms per unit cell
= 8⨯(1/8) + 1 = 2
No. of atoms per unit cell = 2
Coordination no. = 8
Lattice constant = ‘a’
So, length of body diagonal = √3. a = 4r
Atomic radius = (√3. a)/4
This length contains 3 atoms, where no of corner
atoms = 2
Packing fraction =
3
3
4
3
2
r
a
3
3
4 .3 3.
2
3.8.8
a
a
=
3
0.68
8
= =
P.F = 0.68
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14. Face-Centered Cubic Lattice
Unit cell contains 14 atoms, 1 in each corner
and 6 in faces
Each corner atom is shared among 8 cells,
and each face atom is shared among 2 cells,
so total no of atoms per unit cell
= 8⨯(1/8) + 6⨯(1/2) = 4
No. of atoms per unit cell = 4
Coordination no. = 12
Lattice constant = ‘a’
So, length of face diagonal = √2. a = 4r
Atomic radius = 2√2.a
This length contains 3 atoms, where no of corner
atoms = 2
Packing fraction =
3
3
4
3
4
r
a
3
3
4
4
3.16. 2
a
a
= 0.74
3 2
= =
P.F = 0.74
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15. Comparative Study between SC, BCC, FCC
Feature Simple Cubic (SC)
Body-Centered Cubic
(BCC)
Face-Centered Cubic
(FCC)
Atom Locations
Atoms only at the 8
corners of the cube
Atoms at the 8 corners
and 1 atom at the body
center
Atoms at the 8 corners
and at the center of each
of the 6 faces
Atoms per Unit Cell 1 2 4
Coordination Number 6 8 12 (
Relationship between
Edge Length (a) and
Atomic Radius (r)
a = 2r a = 4r/√3 a = 2√2 r
Packing Efficiency (APF) 52.4% 68% 74%
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16. Miller Indices
Position and orientation of a crystal plane is
determined by any three non-collinear points in
the plane. The notation by which the plane is
described, is called Miller Indices.
a2
a
3
a1
u2a2
u
3
a
3
1 1 2 2 3 3
r u a u a u a
= + +
where are translational vectors
1 2 3
, ,
a a a
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17. How to calculate Miller Indices
Determine intercept of each plane along each of
3 crystallographic directions.
Calculate reciprocals of intercepts.
If fraction appears, multiply each by the
denominator of the smallest fraction.
X
Y
Z
X
Y
Z
X
Y
Z
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18. Interplanar Spacing
Perpendicular distance between two adjacent parallel
planes in a crystal lattice is called interplanar spacing
X
Y
Z
P
γ
β
α
O
Plane (hkl) intercepts the coordinate system at
(a/h), (b/k), (c/l) respectively
Interplanar spacing dhkl = OP
cos( )
/
hkl
d
a h
=
cos( )
/
hkl
d
b k
= cos( )
/
hkl
d
c l
=
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19. Interplanar Spacing
X
Y
Z
P
γ
β
α
O
2 2 2
cos ( ) cos ( ) cos ( ) 1
+ + =
2 2 2
1
/ / /
hkl hkl hkl
d d d
a h b k c l
+ + =
2 2 2
2 2 2
1
hkl
d
h k l
a b c
=
+ +
For cubic cell
( )
2 2 2
hkl
a
d
h k l
=
+ +
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