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Static electricity ionic charging

This situation appears to be different when microwave conductivity measurements are used in parallel with electrochemical measurements. As Fig. 1 shows, there is a marked parallelism between electrochemical processes and microwave conductivity mechanisms. In both cases electrical fields interact with electronic or ionic charge carriers as well as dipoles. In electrochemical processes, it is a static or low-frequency electrical field that is moving electrical charge carriers or orienting dipoles. In a micro-wave measurement, the electric field of the microwave interacts with... [Pg.436]

Figure 1. Drawing showing how static electrical fields and microwave fields interact with the same electronic or ionic charge carriers and electrical dipoles. Figure 1. Drawing showing how static electrical fields and microwave fields interact with the same electronic or ionic charge carriers and electrical dipoles.
In this section, a simple description of the dielectric polarization process is provided, and later to describe dielectric relaxation processes, the polarization mechanisms of materials produced by macroscopic static electric fields are analyzed. The relation between the macroscopic electric response and microscopic properties such as electronic, ionic, orientational, and hopping charge polarizabilities is very complex and is out of the scope of this book. This problem was successfully treated by Lorentz. He established that a remarkable improvement of the obtained results can be obtained at all frequencies by proposing the existence of a local field, which diverges from the macroscopic electric field by a correction factor, the Lorentz local-field factor [27],... [Pg.39]

Since static electricity is a surface phenomenon, effective antistatic surface treatments can be used as a means of dissipating static charge. Treatments that give an ionic surface character have been effective [500], Surface treatments employing fatty acids [501], vinyl ether copolymers [502], and quaternary ammonium compounds [503] have all been reported. Other approaches are to incorporate metal or metallized fibers in combination with special conducting backings [504-510]. [Pg.923]

To make things even more complicated, the historical definition of electrostriction, which was developed in physical chemistry already in the late nineteenth century, is given by the Dmde-Nemst equation (Drade and Nemst 1894) and describes the volume contraction AF / in an electric medium of relative static dielectric permittivity upon introduction of an ionic charge with the number z and the effective radius r ... [Pg.502]

The addition of salts modifies the composition of the layer of charges at the micellar interface of ionic surfactants, reducing the static dielectric constant of the system [129,130]. Moreover, addition of an electrolyte (NaCl or CaCli) to water-containing AOT-reversed micelles leads to a marked decrease in the maximal solubihty of water, in the viscosity, and in the electrical birefringence relaxation time [131],... [Pg.485]

The terms in equation 1.166 represent total ionic polarizability, composed of electronic polarizability a plus an additional factor a , defined as a displacement term, due to the fact that the charges are not influenced by an oscillating electric field (as in the case of experimental optical measurements) but are in a static field (Lasaga, 1980) ... [Pg.90]

Here er is the relative -> permittivity (static dielectric constant) of the solution, 0 is the permittivity of free space, e is the unit charge on the electron (- elementary electric charge), 3 is the valence of the ionic species i, Ci is the bulk concentration of the adsorbing species i, k is the Boltzmann constant, T is the absolute temperature, and (V(a)) is the time-averaged value of the electric potential difference across the diffuse layer. The diffuse layer capacitance is (very roughly) of the order of 10 pF cm-2. The thickness of the diffuse layer is essentially the - Debye length Ld,... [Pg.152]

The expression given in Eq. (10) for the work assumes that p = 0, where p is the ionic strength of the medium. AG is the free-energy of the equilibrated excited-state (AG AE00), rD and rA are the molecular radii of the donor and acceptor molecules, e5 is the static dielectric constant or permittivity of the solvent, and z is the charge on each ion. ss is related to the response of the permanent dipoles of the surrounding solvent molecules to an external electrical field. Equation (9), the Bom equation, measures the difference in solvation energy between radical ions in vacuo and solution. [Pg.30]

An applied electric field can be the electric held component of an electromagnetic wave, in which case electronic excitations or other optical responses may ensue. These are the topic of the next chapter. Here, the concern is with electrostatics, specihcally, the dielectric, or insulative, properties of materials. In an electrical conductor, an applied electric held, E, produces an electric current - ions, in the case of an ionic conductor, or electrons, in the case of an electronic conductor. Electrical conductivity has already been examined in earlier chapters. In insulating solids, the topic of the current discussion, the response to an applied electric held is a static spatial displacement of the bound ions or electrons, resulting in an electrical polarization, P, or net dipole moment (charge separahon) per unit volume, which is a vector quantity. In a homogeneous linear and isotropic medium, the polarization and electric held are aligned. In an anisotropic medium, this need not be so. The fth component of the polarization is related to the jth component of the electric held by ... [Pg.364]


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