ee138 chapter 1_slides

14
Chapter 1 1 Outline Reading: Livingston, Chapter 1.1-1.6 Ohm’s Law – Macroscopic – Microscopic Drude’s Model Hydrodynamic Fluid Model Hall Effect Definition and description Free charge carrier density vs. mobility • Temperature • Alloying – Applications

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UCR EE138

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  • Chapter 1 1

    OutlineReading: Livingston, Chapter 1.1-1.6

    Ohms Law Macroscopic Microscopic

    Drudes Model Hydrodynamic Fluid Model Hall Effect

    Definition and description Free charge carrier density vs. mobility

    Temperature Alloying

    Applications

  • Chapter 1 2

    Ohms Law: MacroscopicOhms Law

    Conventions:

  • Chapter 1 33

    Ohms Law: Microscopic

  • Chapter 1 4

    Drudes Model: Free Electron Theory of Metals (1)

    Paul Drude(1863-1906)Credited with the free electron theory of metals

    Kinetic Energy Charged Particle

    e-

    fixed lattice and free electron gas

    electrons are particles collisions with other e-,

    surfaces, lattice random collisions

    http://www.youtube.com/watch?v=dyX5I_io7bg

  • Chapter 1 5

    Drude Model: Free Electron Theory of Metals (2)E

    e-

    e-e-

    e-

    x

    A net e- motion = current

  • Chapter 1 6

    Hydrodynamic Fluid Model: Resistance as Viscosity

    XedtdmmaF =

    +== DD vv

    XedtdmmaF === Dv

    Xem =Dv

    X1vD m

    e= X

    me

    =Dv

    1=No drag:

    With drag:

    If viscosity is so large, terminal velocity is reached and dvD/dt = 0

    then

    compare to

    andincreasing viscosity (decreasing collision time)

    http://www.youtube.com/watch?v=49Kor-zHQM0

  • Chapter 1 7

    Compare Thermal Velocity (vth) to Drift Velocity (vD)

    Calculate vth at room temperature. Calculate vD for a typical metal in an electric field of 1 V/m.

    ~ 5x10-3 m2/V-s

  • Chapter 1 8

    Hall Effect: Definition & Description (1)

    Edwin Hall(1855-1938)Credited with discovering the Hall Effect

    v

    o

    l

    t

    m

    e

    t

    e

    r

    x

    z

    y

    e-e-

    Lorentz Force (FL):

    Hall Field Force (FH):

    (for negative charge carriers)

    Define Hall Coefficient (RH):

  • Chapter 1 9

    Hall Effect: Definition and Description (2)

    Link to applet showing the Hall Effect on negatively charged particles:

    Link to applet showing the motion of negatively and positively charged particles in a magnetic field:

    http://dev.physicslab.org/asp/applets/javaphysmath/java/partmagn/default.asp

    http://jakobvogel.net/go/physics/magnetism/halleffect

  • Chapter 1 10

    Hall Effect: Mobility and Carrier Density (3)

    10

    Why do semiconductors & insulators have higher resistivity than metals?

    Metals SemiconductorsRH independent of T, alloying, defects RH decreases with increasing T and doping

  • Chapter 1 11

    Hall Effect: Applications (4)Hall Probe: Measuring Magnetic Field

    Hall Effect Sensors: Sensing Magnetic Field

    http://www.youtube.com/watch?v=8lPKIaa7Q50

  • Chapter 1 12

    Example:A metal has a collision time of 10-14 s. Find the mean free path at room temperature.

  • Chapter 1 13

    Chapter #1: Review Questions

    1. What is Ohms Law in macroscopic and microscopic terms?

    2. What are the units of conductivity?3. Does the kinetic energy of an electron increase or

    decrease with temperature? 4. Describe the motion of an electron in a metal under an

    applied electric field? What is the mean free path? What is the collision time?

    5. What are the units of mobility?6. What is the Hall Effect? 7. What are some applications of the Hall Effect?

  • Chapter 1 14

    Important Equations

    RIIVP 2==

    IRV =

    LV

    =X

    AIJ =

    ALR =

    X=J

    1= X=Dv

    eNe=

    DeeNJ v=

    me =

    2/13

    =

    mkTvth

    BDH v=X

    eNR

    eH

    1=

    BRHH J=X

    Important ConstantsSpeed of light in vacuum: c = 3.0 x 108 m/sMass of an electron: m = 9.11 x 10-31 kgBoltzmann constant: kB = 1.38 x 10-23 J/KAvogadros Number: NA = 6.022 x 1023 /mole