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Volumn 40, Issue 21, 2007, Pages 7644-7655

Effective interaction parameter for homologous series of deuterated polystyrene-block-poly(n-alkyl methacrylate) copolymers

Author keywords

[No Author keywords available]

Indexed keywords

DIRECTIONAL INTERACTIONS; HOMOLOGOUS SERIES; SIDE GROUPS;

EID: 35549006802     PISSN: 00249297     EISSN: None     Source Type: Journal    
DOI: 10.1021/ma070754z     Document Type: Article
Times cited : (51)

References (54)
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    • Freed and co-workers were the first to incorporate finite compressibility into the incompressible RPA by allowing for vacancy. See: (a) McMullen, W. E, Freed, K. F. Macromolecules 1990, 23, 255;
    • Freed and co-workers were the first to incorporate finite compressibility into the incompressible RPA by allowing for vacancy. See: (a) McMullen, W. E.; Freed, K. F. Macromolecules 1990, 23, 255;
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    • 6625. Other theories have also been formulated using vacancies as a pseudosolvent in the incompressible treatment. See
    • (e) Dudowicz, J.; Freed, K. F. Macromolecules 1995, 28, 6625. Other theories have also been formulated using vacancies as a pseudosolvent in the incompressible treatment. See:
    • (1995) Macromolecules , vol.28
    • Dudowicz, J.1    Freed, K.F.2
  • 33
    • 0032047810 scopus 로고    scopus 로고
    • Pair correlation functions and spinodals from the compressible RPA theories were used to explain LDOT behavior driven by the compressibility difference. Our compressible RPA theory is, however, unique in that it does not depend on the widely used pseudosolvent technique
    • (h) Hino, T.; Prausnitz, J. M. Macromolecules 1998, 31, 2636. Pair correlation functions and spinodals from the compressible RPA theories were used to explain LDOT behavior driven by the compressibility difference. Our compressible RPA theory is, however, unique in that it does not depend on the widely used pseudosolvent technique.
    • (1998) Macromolecules , vol.31 , pp. 2636
    • Hino, T.1    Prausnitz, J.M.2
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    • 26c.
    • 26c.
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    • 6MA.
    • 6MA.
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    • For LDOT-type or loop-forming dPS-b-PAnMA, the following equations were determined to represent the experimental χ L· χL, 1.6128, 118.12/T, 0.2194 lnT for dPS-b-PA2MA; χL, 0.2694, 42.18/T, 0.0279lnT for dPS-b-PA3MA; χL, 0.9681, 64.21/T, 0.1307 lnT or χL, 0.2831, 374.26/T, 182484.2/T2, 2.97/T 3 for a better fit for dPS-b-PA4MA; χL, 0.1626, 8.658/T, 0.0187lnT for dPS-b-PA5MA
    • 5MA.
  • 45
    • 33845958153 scopus 로고    scopus 로고
    • Cho, J. Polymer 2007, 48, 429.
    • (2007) Polymer , vol.48 , pp. 429
    • Cho, J.1
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    • 4th ed, Brandrup, J, Immergut, E. H, Grulke, E. A. Eds. Wiley-Interscience: New York
    • Cho, J.; Sanchez, I. C. In Polymer Handbook, 4th ed.; Brandrup, J.; Immergut, E. H.; Grulke, E. A. Eds. Wiley-Interscience: New York, 1999; p VI/591.
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    • 17 However, the predicted pressure coefficients of the ODT's are quite similar for the two cases.
    • 17 However, the predicted pressure coefficients of the ODT's are quite similar for the two cases.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.