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Field-induced birefringence mechanical orientation

The time course of orientational changes induced by electric fields contains information on the orientation mechanism, and on the electrical and geometrical properties (main dipole axis, length) of the aligning and deorienting molecules. For instance, permanent dipole orientation of a given particle type in the presence of a constant electric field builds up with zero slope and has two modes, whereas the build-up of induced dipole orientation starts with maximum slope and is characterized by only one time constant. The deorientation relaxation of a system of identical particles, after termination of the step pulse, is monophasic, independently of the presence of permanent or induced dipoles. Table 3 summarizes the characteristic features of the rotational kinetics indicated by electric dichroism and birefringence for small perturbations. We see that there are a number of specific relationships to differentiate between permanent and induced dipole mechanism. In particular, the technique of field-reversal is a sensitive indicator for the relative contributions of permanent or induced dipoles. [Pg.166]


See other pages where Field-induced birefringence mechanical orientation is mentioned: [Pg.353]    [Pg.236]    [Pg.151]    [Pg.5358]    [Pg.174]    [Pg.872]    [Pg.1274]    [Pg.123]    [Pg.175]   
See also in sourсe #XX -- [ Pg.553 , Pg.554 , Pg.555 , Pg.556 , Pg.557 , Pg.558 , Pg.559 , Pg.560 , Pg.561 ]




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