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Electric polarization time-dependent

ELECTRIC POLARIZATION OF POLAR TIME-DEPENDENT RIGID MATERIALS... [Pg.217]

ELECTRIC POLARIZATION OF POLAR TIME-DEPENDENT RIGID MATERIALS 233 dyn. The strain energy under these conditions is given by ... [Pg.233]

Electric Polarization of Polar Time-Dependent-Rigid... [Pg.643]

Fig. 4.6. Piezoelectric pulse diagrams can be used to obtain explicit representations of the time dependent electric fields in piezoelectric substances. The magnitudes and orientations of these electric fields are critical to development of shock-induced conduction. As an example, the diagram on the left shows the polarization and displacement relations for a location at the input electrode. The same functions for a location within the crystal is shown on the right (after Davison and Graham [79D01]). Fig. 4.6. Piezoelectric pulse diagrams can be used to obtain explicit representations of the time dependent electric fields in piezoelectric substances. The magnitudes and orientations of these electric fields are critical to development of shock-induced conduction. As an example, the diagram on the left shows the polarization and displacement relations for a location at the input electrode. The same functions for a location within the crystal is shown on the right (after Davison and Graham [79D01]).
In the operation of ferroelectric liquid crystal devices, the applied electric field couples directly to the spontaneous polarisation Ps and response times depend on the magnitude E Ps. Depending on the electronic structure (magnitude and direction of the dipole moment as well as position and polarity of the chiral species) and ordering of the molecules P can vary over several orders of magnitude (3 to 1.2 x 10 ), giving response times in the range 1-100 ps. [Pg.14]

Relaxation processes are probably the most important of the interactions between electric fields and matter. Debye [6] extended the Langevin theory of dipole orientation in a constant field to the case of a varying field. He showed that the Boltzmann factor of the Langevin theory becomes a time-dependent weighting factor. When a steady electric field is applied to a dielectric the distortion polarization, PDisior, will be established very quickly - we can say instantaneously compared with time intervals of interest. But the remaining dipolar part of the polarization (orientation polarization, Porient) takes time to reach its equilibrium value. When the polarization becomes complex, the permittivity must also become complex, as shown by Eq. (5) ... [Pg.9]


See other pages where Electric polarization time-dependent is mentioned: [Pg.1591]    [Pg.88]    [Pg.658]    [Pg.8]    [Pg.283]    [Pg.316]    [Pg.591]    [Pg.273]   
See also in sourсe #XX -- [ Pg.241 , Pg.242 ]




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