Dielectric Spectroscopy

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dielectric spectroscopy

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  • DIELECTRIC SPECTROSCOPY

    &

    Comparison With Other Techniques

  • DIELECTRIC SPECTROSCOPY

    measures the dielectric and electric properties of a medium as a function of frequency (time)

    is based on the interaction of an external electric field with the electric dipole moment and charges of the medium

  • Dielectric properties

    Complex dielectric permittivity relative to vacuum

    *()=()-i()

    Complex conductivity

    *()=()+i()

    Complex electric modulus

    *()=()+i()

    as a function of temperature

  • Medium in an external electric field

    ElectricField

    D=0sE

    D=0E+PP=0sEs= s+1

  • Medium in an external electric field

    Relation between macroscopic and microscopic quantities

    =i

    ipVP 1

    Dipole moments can have an induced or a permanent character

    Permanent dipole moments, Induced polarization, P

    +=+= PVNP

    VP

    ii

    1

    Is determined by:The interaction between the dipolesThe local electric field at the location of the dipole

  • Medium in an external electric field

    EkT3

    2 =

    No interaction between dipoles and local electric field equal to the outer applied fieldthermal energy interaction energy between the dipole and the electric field

    VN

    kTs2

    031

    =

    Interactions between molecules, effect of polarization of environment

    VN

    kTFgs

    2

    031

    =

    ( )( )

    ++

    =

    s

    sF23

    2 2 Internal field Onsager factor

    cos122

    int zg +== Dipole interactions Kirkwood-Froehlich factor

    Onsager-Kirkwood-Froehlich equation

    Langevin equation

    Relation between macroscopic and microscopic quantities

  • Dielectric dispersion in time domain

    PerturbationElectricField

    E(t)(t)

    ResponseElectricDisplacement

    D(t)

    E0

    0

    E(t)

    t

    oo0E0

    0

    D(t)

    t

    0sE0 ( ) ( ) 00 EttD =

    ( ) ( ) ( )tt s +=

    ( ) 00 = ( ) 1=

    ( ) ( )tt = 1

  • Dielectric dispersion in frequency domain

    PerturbationElectricField

    E()*()

    ResponseElectricDisplacement

    D*()

    D(t)=D0sin(t-)

    t

    E(t)=E0sin(t)

    ( ) ( ) ( ) DiDD +=*

    ( ) ( ) cos0DD =

    ( ) ( ) sin0DD =

    ( ) ( )

    cos00

    0

    ED

    =

    ( ) ( )

    sin00

    0

    ED

    =

  • Time-frequency domain

    ( ) [ ]dttidt

    td

    =

    exp)(0

    *( )( ) [ ] pi

    dtidt

    tdexp

    21)(

    0

    *

    =

    ( ) ( )[ ]tt s = 1)(

    ( ) ( ) [ ]dttidt

    tds

    =

    exp)(0

    *

    0)( = t

    ( ) ( ) ( ) ( )2

    020)(

    +

    =