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Volumn 63, Issue 3, 2001, Pages

Fluctuation-entanglement mechanism for director anchoring at nematic polymer surfaces

Author keywords

[No Author keywords available]

Indexed keywords

ANISOTROPY; CRYSTAL STRUCTURE; DAMPING; DEFORMATION; ELASTICITY; HAMILTONIANS; MOLECULAR WEIGHT; NEMATIC LIQUID CRYSTALS; SURFACE TENSION;

FRANK ELASTICITY; POLYMER NEMATICS; SURFACE ANCHORING;

LIQUID CRYSTAL POLYMERS;

EID: 4243457386 PISSN: 1063651X EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevE.63.031708 Document Type: Article

Times cited : (5)

References (13)

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- Yokoyama, H.¹

2
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3
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- Teixeira, P.I.C.¹ Sluckin, T.J.²

4
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- E. M. Del Rio, M. M. Telo da Gama, E. de Miguel, and L. F. Rull, Phys. Rev. E 52, 5028 (1995);
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- Del Rio, E.M.¹ Telo da Gama, M.M.² de Miguel, E.³ Rull, L.F.⁴

5
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- Phys. Rev. EF. N. Braun, T. J. Sluckin, E. Velasco, and L. Mederos, 53, 706 (1996).
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6
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- F. N. Braun, J. Chem. Phys. 111, 4851 (1999).
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9
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10
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- A. Ajdari, B. Duplantier, D. Hone, L. Peliti, and J. Prost, J. Phys. II 2, 487 (1992).
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- Ajdari, A.¹ Duplantier, B.² Hone, D.³ Peliti, L.⁴ Prost, J.⁵

11
- 85035271147
- Onsager’s well-known entropic theory of nematic ordering predicts (see 9) (Formula presented) where d is the cross-sectional diameter and (Formula presented) the axial ratio of the mesogens. The numerical factor (Formula presented) is a function of scaled rod volume fraction (Formula presented) For splay and twist, (Formula presented) (Formula presented) but for bend, (Formula presented) becomes large with increasing scaled volume fraction
- Onsager’s well-known entropic theory of nematic ordering predicts (see 9) (Formula presented) where d is the cross-sectional diameter and (Formula presented) the axial ratio of the mesogens. The numerical factor (Formula presented) is a function of scaled rod volume fraction (Formula presented) For splay and twist, (Formula presented) (Formula presented) but for bend, (Formula presented) becomes large with increasing scaled volume fraction.

12
- 85035270303
- The polydomain structure has been interpreted variously as a consequence of long relaxation times for nematic defects and as a random anisotropy effect originating from entanglements (see 5
- The polydomain structure has been interpreted variously as a consequence of long relaxation times for nematic defects and as a random anisotropy effect originating from entanglements (see 5).

13
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- S.-D. Lee and R. B. Meyer, in Liquid Crystallinity in Polymers, edited by A. Ciferri (VCH, New York, 1991)
- S.-D. Lee and R. B. Meyer, in Liquid Crystallinity in Polymers, edited by A. Ciferri (VCH, New York, 1991).

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