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Volumn 66, Issue 4, 2002, Pages 13-

Elastic properties of polymer interfaces: Aggregation of pure diblock, mixed diblock, and triblock copolymers

Author keywords

[No Author keywords available]

Indexed keywords

AGGLOMERATION; INTERFACES (MATERIALS); LIPIDS; MATHEMATICAL MODELS; MICROEMULSIONS; POLYMER BLENDS; THERMAL EFFECTS;

EID: 41349087460     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.041805     Document Type: Article
Times cited : (40)

References (54)
  • 13
    • 85036405446 scopus 로고    scopus 로고
    • M. Schick, in Liquids at Interfaces Proceeding of Les Houches, Session XLVIII, edited by J. Charvolin, J. F. Joanny, and J. Zinn-Justin (Elsevier, Amsterdam, 1990)
    • M. Schick, in Liquids at Interfaces, Proceeding of Les Houches, Session XLVIII, edited by J. Charvolin, J. F. Joanny, and J. Zinn-Justin (Elsevier, Amsterdam, 1990).
  • 30
    • 85036138652 scopus 로고    scopus 로고
    • If we did not fix the location of the interface explicitly, the system would be unstable in the grand-canonical ensemble, i.e., the equilibrium would be a homogeneous phase
    • If we did not fix the location of the interface explicitly, the system would be unstable in the grand-canonical ensemble, i.e., the equilibrium would be a homogeneous phase.
  • 32
    • 85036396054 scopus 로고    scopus 로고
    • Comparing the saturation line (Formula presented) with the complete phase diagram of the ternary system in Ref. 3, we observe that the saturation line is almost identical to the unbinding transition or the homopolymer-rich phase boundary of the three-phase region
    • Comparing the saturation line (Formula presented) with the complete phase diagram of the ternary system in Ref. 3, we observe that the saturation line is almost identical to the unbinding transition or the homopolymer-rich phase boundary of the three-phase region.
  • 34
    • 0028769234 scopus 로고
    • MacromoleculesA. N. Semenov27, 2732 (1994).
    • (1994) , vol.27 , pp. 2732
    • Semenov, A.N.1
  • 45
    • 85036404153 scopus 로고    scopus 로고
    • This criterion applies only if the interaction between the lamellae is negligible, i.e., when the SCF calculations predict highly swollen lamellar phases or when a minor attractive interaction between the interfaces is overcome by repulsion due to fluctuations. Mixtures of copolymers might also prove useful in tuning the interaction between interfaces 12, which is not considered here
    • This criterion applies only if the interaction between the lamellae is negligible, i.e., when the SCF calculations predict highly swollen lamellar phases or when a minor attractive interaction between the interfaces is overcome by repulsion due to fluctuations. Mixtures of copolymers might also prove useful in tuning the interaction between interfaces 12, which is not considered here.
  • 50
    • 85036203223 scopus 로고    scopus 로고
    • C. Hiergeist, Ph.D. thesis, Universität Potsdam, 1997 (unpublished)
    • C. Hiergeist, Ph.D. thesis, Universität Potsdam, 1997 (unpublished).
  • 51
    • 85036165102 scopus 로고    scopus 로고
    • The segregation of a chain to the interface is controlled by three contributions to the free energy: (i) the loss of translational entropy, (ii) the lowering of the energy by an amount (Formula presented) per chain due to extending the anchoring blocks into the A-rich phase, and (iii) the loss of conformational entropy at the interface. The latter contribution imparts a spontaneous curvature onto the interface. To a first approximation, we conceive the chain conformation of the triblock at the interface as that of individual blocks at an impenetrable surface. Each block suffers an entropy loss of the order (Formula presented) If we increase the size of the middle block (Formula presented) at fixed (Formula presented) the loss of conformational entropy will outweigh the enthalpic contribution for (Formula presented) and the triblock will be repelled from the interface
    • The segregation of a chain to the interface is controlled by three contributions to the free energy: (i) the loss of translational entropy, (ii) the lowering of the energy by an amount (Formula presented) per chain due to extending the anchoring blocks into the A-rich phase, and (iii) the loss of conformational entropy at the interface. The latter contribution imparts a spontaneous curvature onto the interface. To a first approximation, we conceive the chain conformation of the triblock at the interface as that of individual blocks at an impenetrable surface. Each block suffers an entropy loss of the order (Formula presented) If we increase the size of the middle block (Formula presented) at fixed (Formula presented) the loss of conformational entropy will outweigh the enthalpic contribution for (Formula presented) and the triblock will be repelled from the interface.
  • 53
    • 85036207285 scopus 로고    scopus 로고
    • R. Strey (private communication)
    • R. Strey (private communication).
  • 54
    • 85036324613 scopus 로고    scopus 로고
    • C. Frank, Diploma thesis, Universität zu Köln, 2001 (unpublished)
    • C. Frank, Diploma thesis, Universität zu Köln, 2001 (unpublished).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.