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Volumn 12, Issue 1, 2003, Pages 101-110

Viscoelastic dynamics of polymer thin films and surfaces

Author keywords

[No Author keywords available]

Indexed keywords

FREEZING; GLASS TRANSITION; INTERFACES (MATERIALS); MELTING; NEWTONIAN FLOW; PHASE DIAGRAMS; STRAIN; SURFACE TREATMENT; THERMODYNAMIC STABILITY; THIN FILMS; VISCOELASTICITY;

EID: 0345393225     PISSN: 12928941     EISSN: None     Source Type: Journal    
DOI: 10.1140/epje/i2003-10044-4     Document Type: Conference Paper
Times cited : (30)

References (61)
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    • 0345493570 scopus 로고    scopus 로고
    • note
    • The memory kernel discussed here is conceptually different from the memory function of stress, as discussed, e.g., in the context of Lodge liquids [3].
  • 27
    • 0345493569 scopus 로고    scopus 로고
    • note
    • It should be noted, however, that the equation derived by Ronca is not a mode coupling equation per se. Its memory kernel depends explicitly on time, whereas in mode coupling theory, it depends on time only via φ(t). It is not clear yet whether this difference is essential in the case of strain fields.
  • 28
  • 29
    • 0345493568 scopus 로고    scopus 로고
    • PhD Thesis, University of Ulm (1997)
    • G. Eckert, PhD Thesis, University of Ulm (1997).
    • Eckert, G.1
  • 40
    • 0345493566 scopus 로고    scopus 로고
    • Thesis, University of Konstanz (1996) ISBN 3-930803-10-0
    • K. Jacobs, Thesis, University of Konstanz (1996) ISBN 3-930803-10-0.
    • Jacobs, K.1
  • 57
    • 0344199751 scopus 로고    scopus 로고
    • cond-mat/0105065 (2001)
    • D. Podzimek et al., cond-mat/0105065 (2001).
    • Podzimek, D.1
  • 60
    • 0345062052 scopus 로고    scopus 로고
    • ℜ(·) and ℑ(·) denote the real and the imaginary part of their argument, respectively
    • ℜ(·) and ℑ(·) denote the real and the imaginary part of their argument, respectively.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.