atomic structure and interatomic bondingamoukasi/cbe30361/lecture_4_2014_lecture.pdfyoung’s...
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ATOMIC STRUCTURE AND
INTERATOMIC BONDING
Chapter 2
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INTERATOMIC BONDS
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Comparison of Different Atomic Bonds
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INTERATOMIC BONDS (1)
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INTERATOMIC BONDS (2)
FA – attractive force is defined by the nature of the
bond (e.g. Coulomb force for the ionic bonding)
FR – atomic repulsive force, when electron shells
start to overlap
Thus the net force FN (r) = FA + FR
In equilibrium: FN (r0) = FA + FR =0
Let us consider the same conditions
but in the term of potential energy, E.
By definition:
minimum
,0,
00
0
possessesEand
mequilibriuinsystem
Frratlyspecificalmore
extremumhasEdr
dEFif
EEdrFdrFdrFE
FdrE
N
N
NN
N
RA
r r
RA
r
NN
nRr
BE
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F
bonds
stretch
return to
initial
1. Initial 2. Small load 3. Unload
Elastic means reversible!
F Linear-
elastic
Non-Linear-
elastic
ELASTIC DEFORMATION
Strain
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Stress Versus Strain:
Elastic Deformation
Typical Stress-Strain Diagram
for one-dimensional tensile test Elastic Region
Hooke's Law: s = E e
E [N/m2; GPa] is Young’s modulus or modulus of elasticity
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• Bond length, r
• Bond energy, Uo
F F
r
U o = “bond energy”
Energy (r) = U(r)
r o r
unstretched length
PROPERTIES FROM BONDING: E (1)
• Elastic modulus, E
L F
Ao = E
Lo
Elastic modulus
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• Elastic modulus, E
L F
Ao = E
Lo
Elastic modulus
r
larger Elastic Modulus
smaller Elastic Modulus
Energy
ro unstretched length
E is larger if Uo is larger.
PROPERTIES FROM BONDING: E (2)
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Atomic Mechanism of Elastic
Deformation
E~(dF/dr)r o
ro- equilibrium
Weaker bonds – the atoms easily move out from equilibrium position
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r
larger Elastic Modulus
smaller Elastic Modulus
Energy
ro unstretched length
• Elastic modulus, E
• E ~ S=curvature of U at ro
L F
Ao = E
Lo
Elastic modulus
PROPERTIES FROM BONDING: E (3)
The “stiffness” (S) of the bond is given by:
S=dF/dr=d2U/dr2
So(d2U/dr2 )ro
Show that E=(So/r0)
U
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Modulus of Elasticity for Different Metals
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Young’s modulus
Young’s modulus is a numerical constant, named for the 18th-century English
physician and physicist Thomas Young, that describes the elastic properties of a
solid undergoing tension or compression in only one direction.
Higher E – higher “stiffness”
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0.2
8
0.6
1
Magnesium,
Aluminum
Platinum
Silver, Gold
Tantalum
Zinc, Ti
Steel, Ni
Molybdenum
Graphite
Si crystal
Glass-soda
Concrete
Si nitrideAl oxide
PC
Wood( grain)
AFRE( fibers)*
CFRE*
GFRE*
Glass fibers only
Carbon fibers only
Aramid fibers only
Epoxy only
0.4
0.8
2
4
6
10
20
40
6080
100
200
600800
10001200
400
Tin
Cu alloys
Tungsten
<100>
<111>
Si carbide
Diamond
PTFE
HDPE
LDPE
PP
Polyester
PSPET
CFRE( fibers)*
GFRE( fibers)*
GFRE(|| fibers)*
AFRE(|| fibers)*
CFRE(|| fibers)*
Metals
Alloys
Graphite
Ceramics
Semicond
Polymers Composites
/fibers
E(GPa)
109 PaComposite data based on
reinforced epoxy with 60 vol%
of aligned
carbon (CFRE),
aramid (AFRE), or
glass (GFRE)
fibers.
YOUNG’S MODULI: COMPARISON
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HOT TOPIC
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• Coefficient of thermal expansion, a
a is larger if Uo is smaller.
= a(T2-T1) L
Lo
coeff. thermal expansion
PROPERTIES FROM BONDING: a
.
material CTE (ppm/°C)
silicon 3.2
alumina 6–7
copper 16.7
tin-lead solder 27
E-glass 54
S-glass 16
epoxy resins 15–100
silicone resins 30–300 • a ~ symmetry at ro
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Relationships between properties
Expansion coefficient and melting point
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Engineering materials – the same
dependence
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• Melting Temperature, Tm
r
larger T m
smaller T m
Energy (r)
r o
Tm is larger if Uo is larger
PROPERTIES FROM BONDING: TM
*DNA melting temperature The Tm is defined as the temperature in degrees Celsius, at which 50%
of all molecules of a given DNA sequence are hybridized into a double strand
and 50% are present as single strands.
Note that ‘melting’ in this sense is not a change of aggregate state,
but simply the dissociation of the two molecules of the DNA double helix.
The melting point of a solid is the temperature at which it changes state from
solid to liquid at atmospheric pressure.
At the melting point the solid and liquid phase exist in equilibrium.
The Lindemann criterion states that melting is expected when the root mean
square vibration amplitude exceeds a threshold value.
Assuming that all atoms in a crystal vibrate with the same frequency ν,
the average thermal energy can be estimated using the equipartition theorem:
where m is the atomic mass, ν is the frequency, u is the average vibration
amplitude, kB is the Boltzmann constant, and T is the absolute temperature
If the threshold value of u2 is c2a2 where c is the Lindemann constant and
a is the atomic spacing, then the melting point is estimated as
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Relationships between properties
Modulus and melting point
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Engineering materials – the same
dependence
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Ceramics
(Ionic & covalent bonding):
Metals
(Metallic bonding):
Polymers
(Covalent & Secondary):
Large bond energy
large Tm
large E
small a
Variable bond energy
moderate Tm
moderate E
moderate a
Directional Properties
Secondary bonding dominates
small T
small E
large a
SUMMARY: PRIMARY BONDS
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Type
Ionic
Covalent
Metallic
Secondary
Bond Energy
Large!
Variable
large-Diamond
small-Bismuth
Variable
large-Tungsten
small-Mercury
smallest
Comments
Nondirectional (ceramics)
Directional
(semiconductors, ceramics
polymer chains)
Nondirectional (metals)
Directional
inter-chain (polymer)
inter-molecular
SUMMARY: BONDING