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Chapter10 Electrical Properties

Apr 06, 2018

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    Chapter 10 Electrical Properties

    Preet M. Singh

    (404) 894-6641

    [email protected]

    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.