lecture 3 cont
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structure and properties of materialTRANSCRIPT
9/24/2010
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STRUCTURE AND PROPERTIES
OF MATERIALS
The Structure of Crystalline Solids
Lecture _3_Cont.
September 24, 2010 ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
1
CRYSTALLOGRAPHICCrystallography is the experimental science of determining the
arrangement of atoms in solids. In older usage, it is the scientific
study of crystals.
The word "crystallography" is derived from the Greek words
crystallon = cold drop / frozen drop, with its meaning extending
to all solids with some degree of transparency, and graphein =
write.
Crystallography is a tool that is often employed by materials
scientists. In single crystals, the effects of the crystalline
arrangement of atoms is often easy to see macroscopically,
because the natural shapes of crystals reflect the atomic structure.
In addition, physical properties are often controlled by crystalline
defects. The understanding of crystal structures is an important
prerequisite for understanding crystallographic defects.
September 24, 2010
2ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
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CRYSTALLOGRAPHIC
Representation of:
Points
Directions, and In cubic systems
Planes
Calculate linear and planar densities
In Tutorial Session from page 64 to 76
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3ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
SIGNIFICANCE OF CRYSTALLOGRAPHIC
DIRECTIONS AND PLANES
Crystallographic directions are used to indicate aparticular orientation of a single crystal or of an orientedpolycrystalline material;
Metals deform more easily, in directions along which atomsare in closest contact;
It is much easier to magnetize iron in the [100] directioncompared to [111] or [110];
Metals deform along planes of atoms that are most tightlypacked together;
In electronic materials, we need to be sure the substrate isoriented in such way that the thin film can grow on aparticular crystallographic plane.
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
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SINGLE CRYSTAL
September 24, 2010
5ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
A homogenous solid
formed by a repeating,
three-dimensional
pattern of atoms, ions, or
molecules and having
fixed distances between
constituent parts
Single crystal of silicon
USES OF SINGLE CRYSTAL
Monocrystals of silicon and other semiconductors are
important for manufacture of integrated circuit.
Monocrystals of sapphire and other materials are used
for lasers and nonlinear optics.
Monocrystals of fluorite are sometimes used in the
objective lenses of apochromatic refracting telescopes
Monocrystals of metals, especially superalloys, are used
for their special mechanical properties. Turbine blades of
some gas turbines are made of single crystal cast
superalloy.
Monocrystals of copper (crystalline copper) are used for
fine crystalline powders and hi tech.
September 24, 2010
6ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
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SINGLE-CRYSTAL SEMICONDUCTOR WIRE
BUILT INTO AN OPTICAL FIBER
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
ScienceDaily (Mar. 17, 2008) — An
international science team from Penn State
University in the United States and the
University of Southampton in the United
Kingdom has developed a process for growing
a single-crystal semiconductor inside the
tunnel of a hollow optical fiber. The device
adds new electronic capabilities to optical
fibers, whose performance in electronic devices
such as computers typically is degraded by the
interface between the fiber and the device. The
research is important because optical fibers --
which are used in a wide range of technologies
that employ light, including
telecommunications, medicine, computing, and
remote-sensing devices -- are ideal media for
transmitting many types of signals.
Single-crystal semiconductor
wires integrated into
microstructured optical wires.
POLYCRYSTALLINE STRUCTURE
September 24, 2010
8ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
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AMORPHOUS STRUCTURE
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Amorphous solid substance does
not possess long-range order of
atoms positions. Some liquids when
cooled become more and more
viscous and then rigid, retaining
random atom characteristic
distribution.
This state is called under cooled
liquid or amorphous solid.
Common glass, most of Polymers,
glues and some of Ceramics are
amorphous solids. Some of the
Metals may be prepared in
amorphous solid form by rapid
cooling from molten state.
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
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SINGLE VS. POLY CRYSTALS
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Single crystal
Properties vary with direction Anisotropic material
Example of Anisotropy: BCC iron
Anisotropy (not
isotropic) is the
property of being
directionally
dependent.
SINGLE VS. POLY CRYSTALS
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Poly-crystals
Properties may/may not vary with direction
Example: Common steel is polycrystalline
If grains are random Isotropic E ≈ 210 GPa
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Definitions
Study well the following:
Polymorphism page 61 Example
Allotropy page 61 Iron -Tin
Isotropy and Anisotropy page 82
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Polymorphism is a physical phenomenon where
a material may have more than one crystal
structure. A material that shows polymorphism
exists in more than one type of space lattice in
the solid state. If the change in structure is
reversible, then the polymorphic change is
known as allotropy.
Polymorphism and Allotropy
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
One familiar example is found in
carbon: graphite is the stable
polymorph at ambient conditions,
whereas diamond is formed at
extremely high pressures.
Example (Polymorphism)
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
Diamond and
graphite are two
allotropes of carbon:
pure forms of the
same element that
differ in structure.
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
a) Diamond,
b) Graphite,
c) Lonsdaleite,
d) C60
(Buckminsterfullere
ne or buckyball),
e) C540,
f) C70,
g) Amorphous carbon,
h) single-walled
carbon nanotube or
buckytube.
Eight allotropes of carbon:
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ENGR 230
Structure and Properties of Materials
Nahid Abdel Salam
The best known example for allotropy
is iron. When iron crystallizes at
1538°C it is B.C.C. (δ-iron), at 1394°C
the structure changes to F.C.C. (γ-iron
or austenite), and at 912°C it again
becomes B.C.C. (α-iron or ferrite).
Example (Allotropy)