Crystal Structures and Types of Solids in Materials Science

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PROF. DR. B. J. LOKHANDE
SCHOOL OF PHYSICAL SCIENCES
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In 
a 
Crystalline 
solid
, atoms are 
arranged  in 
an 
orderly
manner. The atoms 
are  
having long range
 
order.
Example 
: 
Iron, Copper and other 
metals,  
NaCl
 
etc.
In 
an 
Amorphous 
solid
, 
atoms 
are not  
present 
in an orderly
manner. They are  
randomly
 
arranged.
Example 
:
 
Glass
Non 
dense, 
random
 
packing
Dense, 
regular
 
packing
r
Energy
typical
 
neighbor
bond
 
length
typical
 
neighbor
bond
 
energy
En
e
r
g
y
r
typical
 
neighbor
bond
 
length
typical neighbor
bond
 
energy
 
 
 
Dense, 
regular-packed 
structures 
tend 
to 
have 
lower
 
energy.
E
N
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R
G
Y
 
A
N
D
 
P
A
C
K
I
N
G
S
O
M
E
 
D
E
F
I
N
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T
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Crystalline
 
material is 
a 
material comprised 
of 
one 
or 
many 
crystals. 
In
 
crystal,
atoms or 
ions 
show 
a 
long-range periodic
 
arrangement.
Single 
crystal 
is 
a 
crystalline 
material 
that 
is made of 
only 
one 
crystal 
(
 no grain
boundaries).
Grains
 
are the crystals in 
a 
polycrystalline
 
material.
Polycrystalline 
material 
is 
a 
material comprised 
of 
many crystals (
single-crystal
material 
that 
has 
only 
one
 
crystal).
Grain boundaries 
are 
regions 
between 
grains of 
a 
polycrystalline
 
material
.
A 
unit 
cell 
is the smallest part of the 
unit cell,  
which when 
repeated 
in 
all three
directions,  reproduces the
 lattice
.
All 
unit cells may 
be 
described
 
via  these vectors 
and angles.
U
N
I
T
 
C
E
L
L
S
 
A
N
D
 
U
N
I
T
 
C
E
L
L
 
V
E
C
T
O
R
S
U
N
I
T
 
CE
L
L
 
OF
 
BCC
LA
T
T
I
CE
F
e
 
(
U
p
 
t
o
 
91
0
0
 
C
 
an
d
 
f
r
o
m
 
14
0
1
0
C
 
to
Melting Point), 
W, 
Cr, 
V,
 
\
UNIT CELL 
OF 
FCC
LATTICE
Al, 
Cu, 
Ni, 
Fe 
(910
0 
C-1401
0
 
C)
UNIT CELL 
OF 
HEXAGONAL CLOSED PACKED
 
(HCP)
Zn,
 
Mg
M
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L
E
R
 
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N
D
I
C
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S
Miller Indices are used to 
represent 
the directions and  the
planes 
in a crystal
Miller Indices is a 
group 
of 
smallest 
integers 
which 
represent a
direction or a plane
z
y
z
[1
 
1
 
1]
[
0
1
2
]
x
[
0
2
1]
y
[111]
[100]
[
11
0
]
b
x
M
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Select any point on the direction line other than the origin Find out the
coordinates of the point in terms of the unit vectors along different axes.
Specify negative coordinate with a bar on top  Divide the m by the unit vector
along the respective axis.
Convert the result into the smallest integers by suitable multiplication or
division.
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Crystal structures in materials science involve the arrangement of atoms in solids, with examples of crystalline and amorphous solids like metals and glass. Explore concepts like energy packing, definitions of crystalline materials, unit cells, BCC and FCC lattices, HCP structures, and Miller Indices in crystallography.

  • Materials Science
  • Crystal Structures
  • Solids
  • Unit Cells
  • Crystallography

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  1. CRYSTAL STRUCTURE PROF. DR. B. J. LOKHANDE SCHOOL OF PHYSICAL SCIENCES

  2. TYPES OF SOLIDS In a Crystalline solid, atoms are arranged in an orderly manner. The atoms are having long range order. Example : Iron, Copper and other metals, NaCl etc. In an Amorphous solid, atoms are not present in an orderly manner. They are randomly arranged. Example : Glass

  3. ENERGY AND PACKING Non dense, randompacking Energy typical neighbor bond length typical neighbor bond energy r Energy Dense, regular packing typical neighbor bond length r typical neighbor bond energy Dense, regular-packed structures tend to have lower energy.

  4. SOME DEFINITIONS Crystalline material is a material comprised of one or many crystals. Incrystal, atoms or ions show a long-range periodic arrangement. Single crystal is a crystalline material that is made of only one crystal (no grain boundaries). Grains are the crystals in a polycrystalline material. Polycrystalline material is a material comprised of many crystals (single-crystal material that has only one crystal). Grain boundaries are regions between grains of a polycrystalline material. A unit cell is the smallest part of the unit cell, which when repeated in all three directions, reproduces the lattice.

  5. UNIT CELLS AND UNIT CELL VECTORS All unit cells may be described via these vectors and angles.

  6. UNIT CELLOF BCC LATTICE Fe (Up to 9100C and from 14010C to Melting Point), W, Cr, V, \

  7. UNIT CELL OF FCC LATTICE Al, Cu, Ni, Fe (9100 C-14010C)

  8. UNIT CELL OF HEXAGONAL CLOSED PACKED (HCP) Zn, Mg

  9. MILLER INDICES Miller Indices are used to represent the directions and the planes in a crystal Miller Indices is a group of smallest integers which represent a direction or a plane y z y z x [021] [111] [012] [111] x [100] [110] b

  10. MILLER INDICES Select any point on the direction line other than the origin Find out the coordinates of the point in terms of the unit vectors along different axes. Specify negative coordinate with a bar on top Divide the m by the unit vector along the respective axis. Convert the result into the smallest integers by suitable multiplication or division.

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