메뉴 건너뛰기




Volumn 53, Issue 3, 1996, Pages 2412-2422

Electro-optic properties of a polymer-dispersed liquid-crystal film: Temperature dependence and phase behavior

Author keywords

[No Author keywords available]

Indexed keywords

BIREFRINGENCE; BOUNDARY CONDITIONS; ELECTRIC FIELDS; ELECTRIC PROPERTIES; FILMS; LIQUID CRYSTALS; MATHEMATICAL MODELS; OPTICAL MICROSCOPY; OPTICAL PROPERTIES; PHASE DIAGRAMS; PHASE TRANSITIONS; THERMAL EFFECTS;

EID: 0030102361     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/physreve.53.2412     Document Type: Article
Times cited : (88)

References (31)
  • 6
    • 0001381848 scopus 로고
    • edited by B. Bahadur World Scientific, Teaneck, NJ, Chap. 14
    • J. W. Doane, in Liquid Crystals: Applications & Uses, edited by B. Bahadur (World Scientific, Teaneck, NJ, 1990), Vol. 1, Chap. 14.
    • (1990) Liquid Crystals: Applications & Uses , vol.1
    • Doane, J.W.1
  • 22
    • 5344225410 scopus 로고    scopus 로고
    • Darmstadt, Germany (EM Industries in the United States)
    • E. Merck, Darmstadt, Germany (EM Industries in the United States).
    • Merck, E.1
  • 23
    • 5344230842 scopus 로고    scopus 로고
    • Norland Products, Inc., New Brunswick, New Jersey
    • Norland Products, Inc., New Brunswick, New Jersey.
  • 27
    • 5344246797 scopus 로고    scopus 로고
    • Personal communication with Dr. Frank Allen of EM Industries, Inc.
    • Personal communication with Dr. Frank Allen of EM Industries, Inc.
  • 29
    • 85087581238 scopus 로고    scopus 로고
    • -2 over a 100-K temperature change. This is far less than the asphericity of the droplets, and so it is not a significant factor. It is for this reason that I am able to ignore thermal expansion effects on drop shape
    • -2 over a 100-K temperature change. This is far less than the asphericity of the droplets, and so it is not a significant factor. It is for this reason that I am able to ignore thermal expansion effects on drop shape.
  • 30
    • 5344221739 scopus 로고    scopus 로고
    • The surface tension approaches zero at a critical point. However, the birefringence data shown in Fig. 7 indicate that the nematic-to-isotropic phase transition is strongly first order. For this reason, the surface tension is presumed to remain large even near the phase transition temperature
    • The surface tension approaches zero at a critical point. However, the birefringence data shown in Fig. 7 indicate that the nematic-to-isotropic phase transition is strongly first order. For this reason, the surface tension is presumed to remain large even near the phase transition temperature.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.