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Electromechanical: behavior measurement

Polarization which can be induced in nonconducting materials by means of an externally appHed electric field is one of the most important parameters in the theory of insulators, which are called dielectrics when their polarizabiUty is under consideration (1). Experimental investigations have shown that these materials can be divided into linear and nonlinear dielectrics in accordance with their behavior in a realizable range of the electric field. The electric polarization PI of linear dielectrics depends linearly on the electric field E, whereas that of nonlinear dielectrics is a nonlinear function of the electric field (2). The polarization values which can be measured in linear (normal) dielectrics upon appHcation of experimentally attainable electric fields are usually small. However, a certain group of nonlinear dielectrics exhibit polarization values which are several orders of magnitude larger than those observed in normal dielectrics (3). Consequentiy, a number of useful physical properties related to the polarization of the materials, such as elastic, thermal, optical, electromechanical, etc, are observed in these groups of nonlinear dielectrics (4). [Pg.202]

The semiconducting properties of the compounds of the SbSI type (see Table XXVIII) were predicted by Mooser and Pearson in 1958 228). They were first confirmed for SbSI, for which photoconductivity was found in 1960 243). The breakthrough was the observation of fer-roelectricity in this material 117) and other SbSI type compounds 244 see Table XXIX), in addition to phase transitions 184), nonlinear optical behavior 156), piezoelectric behavior 44), and electromechanical 183) and other properties. These photoconductors exhibit abnormally large temperature-coefficients for their band gaps they are strongly piezoelectric. Some are ferroelectric (see Table XXIX). They have anomalous electrooptic and optomechanical properties, namely, elongation or contraction under illumination. As already mentioned, these fields cannot be treated in any detail in this review for those interested in ferroelectricity, review articles 224, 352) are mentioned. The heat capacity of SbSI has been measured from - 180 to -l- 40°C and, from these data, the excess entropy of the ferro-paraelectric transition... [Pg.410]

Anomalous slope of x or e in the vicinity of the phase transition is a reason for the anomalous behavior also for quantities d,e,c, s (tensor indexes are omitted for simplicity) measured at constant electric field. It follows from the thermodynamic relations between the electromechanical coefficients shown in Table 4.3. On the contrary, no anomaly in the temperature dependencies for quantities g,h,cP,P measured at constant electric displacement D (or constant polarization P) is observed. [Pg.89]


See other pages where Electromechanical: behavior measurement is mentioned: [Pg.179]    [Pg.428]    [Pg.87]    [Pg.460]    [Pg.489]    [Pg.313]    [Pg.71]    [Pg.125]    [Pg.114]    [Pg.328]    [Pg.750]    [Pg.862]    [Pg.522]   
See also in sourсe #XX -- [ Pg.441 ]




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