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Dipole dielectric properties

The same idea was actually exploited by Neumann in several papers on dielectric properties [52, 69, 70]. Using a tin-foil reaction field the relation between the (frequency-dependent) relative dielectric constant e(tj) and the autocorrelation function of the total dipole moment M t] becomes particularly simple ... [Pg.11]

Some electrical properties are shown in Table 3. Values of other parameters have been pubflshed (146). Polymorphism of the PVDF chains and the orientation of the two distinct dipole groups, —CF2— and —CH2—, rather than trapped space charges (147) contribute to the exceptional dielectric properties and the extraordinarily large piezoelectric and pyroelectric activity of the polymer (146,148,149). [Pg.387]

The dielectric properties of most foods, at least near 2450 MH2, parallel those of water, the principal lossy constituent of food (Fig. 1). The dielectric properties of free water are well known (30), and presumably serve as the basis for absorption in most foods as the dipole of the water molecule interacts with the microwave electric field. By comparison, ice and water of crystaUi2ation absorb very Httie microwave energy. Adsorbed water, however, can retain its Hquid character below 0°C and absorb microwaves (126). [Pg.344]

The dielectric properties of polar materials will depend on whether or not the dipoles are attached to the main chain. When they are, dipole polarisation will depend on segmental mobility and is thus low at temperatures below the glass transition temperatures. Such polymers are therefore better insulators below the glass temperature than above it. [Pg.117]

In contrast with Eq. (5), Eq. (11) gives the frequency behavior in relation to the microscopic properties of the studied medium (polarizability, dipole moment, temperature, frequency of the field, etc). Thus for a given change of relaxation time with temperature we can determine the change with frequency and temperature of the dielectric properties - the real and imaginary parts of the dielectric permittivity. [Pg.12]

The nonlinear optical and dielectric properties of polymers find increasing use in devices, such as cladding and coatings for optical fibres, piezoelectric and optical fibre sensors, frequency doublers, and thin films for integrated optics applications. It is therefore important to understand the dielectric, optical and mechanical response of polymeric materials to optimize their usage. The parameters that are important to evaluate these properties of polymers are their dipole moment polarizability a, hyperpolarizabilities 0... [Pg.235]

We have shown in this paper the relationships between the fundamental electrical parameters, such as the dipole moment, polarizability and hyperpolarizability, and the conformations of flexible polymers which are manifested in a number of their electrooptic and dielectric properties. These include the Kerr effect, dielectric polarization and saturation, electric field induced light scattering and second harmonic generation. Our experimental and theoretical studies of the Kerr effect show that it is very useful for the characterization of polymer microstructure. Our theoretical studies of the NLDE, EFLS and EFSHG also show that these effects are potentially useful, but there are very few experimental results reported in the literature with which to test the calculations. More experimental studies are needed to further our understanding of the nonlinear electrooptic and dielectric properties of flexible polymers. [Pg.243]

Dibenzothiophene is one of many compounds studied for scintillation counting behavior. The dielectric properties and dipole moment of dibenzothiophene have been recorded. Some discrepancy regarding the dipole moment arose in earlier measurements however, the recent value of 0.84 + 0.05 D, as compared with that of 0.53 D possessed by thiophene, agrees with predictions which have been made based on the relative ease of oxidation of these two compounds. The 7T- and CT-components of the dipole moment have been calculated and found to give an overall moment of 0.93 D, which compares favorably with the experimental value given above. The dipole moments of... [Pg.220]

The dipole, the oetupolar moment and the polarizability of protonated dpg molecules, and therefore the optieal and dielectric properties of dpg salts, depend on the orientation of the rings, whieh justifies the need to determine aecurate struetural data for these eompounds. At the present time sufficient structures have been reported so that eommon conformations or patterns can be identified. Table 7 eontains a brief identification of all the struetures analyzed in this review. [Pg.115]

The induced dipole moment of a polymer in an electric field is proportional to the strength of the field, and the proportionality constant is related to the polarizability of the atoms in the polymer. The dielectric properties of polymers are affected adversely by the presence of moisture, and this effect is greater in hydrophilic than in hydrophobic polymers. [Pg.79]

Collision-induced dipoles manifest themselves mainly in collision-induced spectra, in the spectra and the properties of van der Waals molecules, and in certain virial dielectric properties. Dipole moments of a number of van der Waals complexes have been measured directly by molecular beam deflection and other techniques. Empirical models of induced dipole moments have been obtained from such measurements that are consistent with spectral moments, spectral line shapes, virial coefficients, etc. We will briefly review the methods and results obtained. [Pg.153]

The dielectric properties of gases are closely related to collision-induced absorption. It is well known that collisions modify molecular properties. Specifically, we are here interested in the dipole moments induced by collisions (Chapter 4) which manifest themselves not only in collision-induced absorption, but also in the dielectric virial properties of gases. [Pg.370]

Dielectric Properties. If the linear lattice has a charge of +eon one end and a charge of — e on the other, the polarization per chain is directly proportional to the mean extension (2). This example relates to the special physical case where there exist monomer level dipole components that add up in such a manner that the total chain moment correlates exactly with the end-to-end length. Calculations similar to those of Onishi and Yamamoto (71) lead to the following result for the dielectric constant ... [Pg.108]

In polymer theory, the LDT result corresponds to the theory of large chain extensions P. J. Flory, Statistical Mechanics of Chain Molecules, Interscience, New York, 1969. Another mapping exists onto Debye s theory for dielectric properties of molecules with permanent dipoles P. Debye, Polar Molecules, reprinted, Dover, New York, 1958. [Pg.336]

Steady-State Fluorescence. The fluorescence characteristics of PRODAN are extremely sensitive to the physicochemical properties of the solvent (38). As benchmarks, the steady-state emission spectra for PRODAN in several liquid solvents are presented in Figure 1. It is evident that the PRODAN emission spectrum red shifts with increasing solvent polarity. This red shift is a result of the dielectric properties of the surrounding solvent and the large excited-state dipole moment (ca. 20 Debye units) of PRODAN (38). It is the sensitivity of the PRODAN fluorescence that will be used here to investigate the local solvent composition in binary supercritical fluids. [Pg.100]


See other pages where Dipole dielectric properties is mentioned: [Pg.9]    [Pg.10]    [Pg.237]    [Pg.149]    [Pg.482]    [Pg.344]    [Pg.250]    [Pg.290]    [Pg.31]    [Pg.103]    [Pg.266]    [Pg.197]    [Pg.13]    [Pg.19]    [Pg.21]    [Pg.4]    [Pg.85]    [Pg.6]    [Pg.3]    [Pg.119]    [Pg.446]    [Pg.163]    [Pg.164]    [Pg.356]    [Pg.149]    [Pg.7]    [Pg.4]    [Pg.137]    [Pg.179]    [Pg.241]    [Pg.232]    [Pg.52]    [Pg.55]    [Pg.202]   
See also in sourсe #XX -- [ Pg.231 ]

See also in sourсe #XX -- [ Pg.231 ]




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