Among the various new directions in modern polymer science, the design
and investigation of liquid crystal (LC) polymers have been the ones
growing most actively and fruitfully. In spite of that, the possible
formation of an anisotropic LC phase was only demonstrated theoretically
for the first time in the 1950s by Onsager [1] and Flory [2], and
then experimentally verified in the studies with polypeptides solutions.
In essence, the studies of these LC lyotropic systems did not deviate
from the theme of purely academic interest. It was at the beginning of
the 1970s that the experimental "explosion" occurred, when aromatic
polyamides were synthesized and their ability to form LC solutions in
certain very aggressive solvents was discovered. The search for
practical applications of such LC systems was crowned with the
successful creation of the new generation of ultrastrong high-modulus
ther- mostable fibers, such as the Kevlar, due to the high degree of
order of the macromolecules in the anisotropic LC state. In fact, these
investigations coincided with the swift emergence on the practical
"scene" of thermotropic low-molar-mass liquid crystals, with the use of
these materials in microelectronics and electro optics (figures and let-
ters indicators, displays in personal computers, and flat TV, etc.).
Polymer scientists also began to develop methods of synthesizing
thermotropic LC polymers by incorporating mesogenic fragments in the
main (main-chain LC polymers) or side branchings of the macromolecules
(side-chain or comb- shaped polymers).