LIQUID-CRYSTALS WITH VARIABLE DEGREE OF ORIENTATION
LIQUID-CRYSTALS WITH VARIABLE DEGREE OF ORIENTATION
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DOI:
10.1007/bf00380413
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发表时间:
1991-01-01
影响因子:
2.5
通讯作者:
ERICKSEN, JL
中科院分区:
文献类型:
--
作者:
ERICKSEN, JL
For the small-molecule nematic liquid crystals commonly used in display devices, what CHANDRASE~ ZHAR [1] calls the Oseen-Z6cher-Frank equations, hereafter referred to as the OZF equations, have been quite successful in describing many static phenomena. For phenomena involving flow, what he calls the Ericksen-Leslie equations have been used rather successfully: they reduce to the OZF equations for statics. Many workers accept what he calls Parodi's relation, an Onsager relation. Careful experimental tests of this have not been made, as far as I know. CURRIE [2] points out that it does have some status as a stability condition. Kuzuu & DoI [3] note that the type of molecular theory which they consider does imply this relation. I follow DE GENNES [4] in referring to the resulting equations as the EL or ELP theory, depending on whether Parodi's relation is presumed to hold.Two things have motivated me to consider modifying the equations. For one thing, I am interested in seeing the development of a mathematically sound theory of defects which might be at rest, or moving. The static theory of point defects, based on the OZF equations, is now rather well developed, as is discussed in surveys by ERICKSEN [5] and KINDERLEHRER [6]. I believe that the EL and ELP theories are capable of describing moving point defects. However, no real progress has been made in developing pertinent analyses, despite some serious efforts. More serious difficulties are encountered with some observed kinds of disclinations (line defects). According to the aforementioned theories, these more violent singularities cause energy integrals, etc., to diverge. In dealing with rather specific situations, workers have patched up the theory by excluding a tube of small radius, assigning a finite" core energy" to it. I just do not believe that one can use such ideas as a basis for developing satisfactory mathematical theory, particularly for moving defects. Such phenomena are of interest for both nematic and cholesteric liquid crystals. In the latter, they are associated with the interesting" blue phases" discussed by CLADIS [7] and SETHNA [8], among other things. In tinkering with theories which work rather well, there is some danger that, in fixing one flaw, one will find other good predictions affected adversely. Slowly, I have come to the view that the risk is worth taking. There is a physically reason-