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Chapter 10 Electrical Properties
Preet M. Singh
(404) 894-6641
MSE 2001
Chapter 10 Electrical Properties
Electrical Conduction
Charge per carrier
Mobility
Energy bands and number of charge carriers
Conductors, semiconductors and insulators
Ionic conduction
Conducting polymers
Superconductivity Semiconductors
Intrinsic and extrinsic conduction
Role of defects
Simple devices
Microelectronics
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Electrical Conduction
V = IR
Ohms Law
Positive
potential
Negative
potential
AR
L
1
Resistivity conductivity
Electrical conductivities for a variety of materials at rootemperature
Metals and alloys [( -cm)-1]Al 3.8 x 10
5
Ag 6.3 x 105
Au 4.3 x 105
Co 1.6 x 105
Cr 7.8 x 104
Cu 6.0 x 105
Fe 1.0 x 105
Mg 2.2 x 105
Ni 1.5 x 105
Pd 9.2 x 104
Pb 4.8 x 104
Pt 9.4 x 104
Sn 9.1 x 104
Ta 8.0 x 104
Zn 1.7 x 105
Zr 2.5 x 104
Plain carbon steel (1020) 1.0 x 105
Stainless steel (304) 1.4 x 104
Gray cast iron 1.5 x 104
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Electrical conductivities for a variety of
materials at room temperature
Ceramics [(-cm)-1]ReO3 5.0 x 10
5
CrO2 3.3 x 104
SiC 1.0 x 10-1
Fe3O4 1.0 x 102
SiO2
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Conductivity Depends on
The number of mobile charge carriers per
unit volume (N with units of m-3)
Charge per Carrier, q (units of C)
The mobility of the charge,, with unitsm2/(V-s)
Nq
Charge Carriers
Electrons (metals and some covalent bonds), q
Ions (ionic solids), then q = qe * Z
Z is the valence of the ion
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Collisions
Charge Mobility, Same as diffusion driven by charge gradient
Charge Mobility
E
vor
,
mobilityelectronisWhere
strengthfieldelectrictoalproportionis
fieldappliedtodueonacceleratiofmagnitudeSince
Ev
or
Ev
tavVelocityDrift
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Charge
Mobility
Thermal vibrations
Foreign atomsVacancies
0
T
0
dN
The Influence of Alloying on Conductivity
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The Influence of Cold Work on Conductivity
Increasing electronegativity,increased tendency to add electrons
Increasingatomicradius
Alkalimetals
Alkalineearth
metals
Halogens
Noble
gases
6C
14Si
32Ge
sp3 hybridized orbitals
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Energy,eV
Energy-level diagram for the orbital electrons in a 12C atom.
Primary Bonds
Na
Na+
rNa = 0.186nm
rCl = 0.107nm
rNa = 0.098nm+
rCl = 0.181nm-
Cl
Cl-Ionization
potential
Electron
affinity
Energy required: 5.14 eV Energy released: 4.02 eV
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Metallic Bond
Ion cores of
2+ charge
Delocalized cloud
of valence electrons
Schematic of metallic bonds in solid magnesium
Atomic Structure
Energy
Principal quantum number, n1 2 3 4 5 6 7
s
ps
ps
ps
ps
ps
ps
d
d
d
d
df
f
f
Schematic representation of
the relative energies of the
electrons for the various shellsand subshells.
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Energy Bands in Solids
The permissible energy levels
are a function of separation
distance. Discrete energy levels in the
isolated atoms spread intobands in the solid.
Outermost atoms no longerspatially localized to a particularatom.
The energy bands becomewider as the amount of overlapincreases.
The higher the energy level, thewider the corresponding energyband.
The number of energy levels inan energy band equals thenumber of atoms in the solidmultiplied by the number ofdiscrete energy states in anisolated atom.
Energy Bands in Solids
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Energy Bands in Solids
Energy Bands in Solids
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Electron Distributions in an Energy Band
N = 2 N = 0 N = 2
Sparsely filled Nearly filledCompletely filled
Electron Distribution in a Sparsely Filled Energy BandOriginalemptyResulting hole
after jump
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Electron Distribution in a Partially Filled Band as
a Function of Temperature
T = 0K T1 > 0K T2 > T1
Fermi-Dirac Statistics
1
exp 1f
f EE E
kT
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Effect of Temperature on theDistribution of Electrons in aPartially Filled Electron Band
Permissible by Fermi-Diracbut not allowed since in
band gap N = 0
Energy Distribution for Solids with a Band Gap
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Energy Distribution for Solids with a Band Gap
Permissible byboth Fermi-Dirac
and band structure
Charge carrier
Hole invalence
band
Charge carrier
Energy Distribution for Solids with a Band Gap
kT
E
oe
g
NN2
expNumber of Electrons in Conduction Band
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Energy Band Diagram for Three Classes of
Electrical Materials At 0K
Conductor Semiconductor Insulator
Electron Band Structure for Solid Sodium
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Electron Band Structure for Solid Magnesium
Reference
ConductorTemperature
(C) o(-cm) e (C-1)Al 20 2.65 x 10-6 0.0043
Ag 20 1.59 x 10-6
0.0041
Au 20 2.35 x 10-6 0.0040
Co 20 6.24 x 10-6 0.0060
Cr 0 1.29 x 10-5 0.0030
Cu 20 1.67 x 10-6 0.0068
Fe 20 9.71 x 10-6 0.0065
Mg 20 4.45 x 10-6 0.0065
Ni 20 6.84 x 10-6 0.0069Pd 20 1.08 x 10
-50.0038
Pb 20 2.06 x 10-5
0.0034
Pt 20 1.06 x 10-5 0.0039
Sn 0 1.10 x 10-5 0.0047
Ta 25 1.25 x 10-5 0.0038
Zn 20 5.92 x 10-6 0.0042
Zr 20 4.00 x 10-5 0.0044
TTeo 1)(
Resistivity at Temp (T)
o= Resistivity at a
Reference Temperature
e= Temp. Coefficient of
Resistivity
T = T-T Reference
Effect of Temperature on Electrical Resistivities of selected conductors
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Temperature Measurement by a Thermocouple
SemiconductorsIntrinsic and Extrinsic Conductivities
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Intrinsic Conductivity of Semiconductor
hheee NNq
Conductivity of Semiconductors (when Ionic Conduction in Negligible)
heee qN or
kT
E
oe
g
NN2
expFor band gap materials
kT
E
heeo
g
qN2
exp
kT
E
o
g
2exp heeoo qN Where
Tk
Ego
1
2lnln or
Intrinsic Conductivity of Semiconductor
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Effect of Doping
Effect of Doping
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Effect of Doping
Effect of Defects
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Superconductivity
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Homework Assignment(Not to be turned-in)
2, 5, 6, 7, 8, 9, 10, 11, 12, 13, 15, 16, 18, 19,23, 24, 25, 34, 36, 37, 38, 39, 43, 46, 47, 54,& 57.