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Volumn 106, Issue 12, 1997, Pages 5171-5180

The conformation of hard-sphere polymers in hard-sphere solution calculated by single-chain simulation in a many-body solvent influence functional

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; CONFORMATIONS; INTEGRAL EQUATIONS; MONOMERS; MONTE CARLO METHODS; PROBABILITY; SOLVENTS; THERMODYNAMICS;

EID: 0031097286     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.473560     Document Type: Article
Times cited : (26)

References (45)
  • 7
    • 0001650720 scopus 로고
    • D. Chandler, Y. Singh, and D. M. Richardson, J. Chem. Phys. 81, 1975 (1984); Y. Singh, J. Phys. A 20, 3949 (1987).
    • (1987) J. Phys. A , vol.20 , pp. 3949
    • Singh, Y.1
  • 8
    • 84950583715 scopus 로고
    • edited by J.-P. Hansen, D. Levesque, and J. Zinn-Justin North-Holland, Amsterdam
    • D. Chandler, in Liquids, Freezing and Glass Transition: Les Houches Session LI, edited by J.-P. Hansen, D. Levesque, and J. Zinn-Justin (North-Holland, Amsterdam, 1991), part I, p. 195.
    • (1991) Liquids, Freezing and Glass Transition: Les Houches Session LI , Issue.1 PART , pp. 195
    • Chandler, D.1
  • 29
    • 5644259964 scopus 로고    scopus 로고
    • note
    • An interesting extension of this model for which the SPT potential works without modification is that of pearl-necklace polymers with a local bending potential between neighboring bonds, i.e., model semiflexible polymers.
  • 31
    • 85086527539 scopus 로고    scopus 로고
    • note
    • -6.
  • 40
    • 5644239970 scopus 로고    scopus 로고
    • note
    • A more precise statement is that the diagrams in the virial expansion of the solvation potential that involve three or more monomer root points which are not articulation points are not ignored, but are rather replaced with sets of topologically similar "screening" diagrams which are articulable into diagrams with only two root points. For a less cryptic discussion please see References 16 and 18.
  • 42
    • 5644293471 scopus 로고    scopus 로고
    • note
    • N which illustrates this point is in Ref. 16.
  • 44
    • 5644254779 scopus 로고    scopus 로고
    • note
    • The surface tension of a real high-density fluid, which also exhibits the layering behavior, is positive because of the contribution from the long-range attractive potential, which overwhelms the negative "packing" contribution. However, in adapting the SPT potential to work with molecules with attractions, one would probably not want to include this contribution to the surface tension used in Eq. (10). The reason is that this contribution originates from long range attractions, and the cavity created by the monomer is smaller than the range of these interactions. That is, on the length scale of the attractions insertion of the monomer requires creation of "zero" new surface in the solvent.
  • 45
    • 5644231186 scopus 로고    scopus 로고
    • note
    • We worked out similar formulas for p = 3 and p = 4 in the hopes that perhaps for s = b no more than four shadows could ever mutually overlap on the unit sphere. Unfortunately a short numerical study showed that this is not the case. Since after p = 4 imagining all the ways p circles can overlap on the surface of a sphere is difficult, we constructed instead a general but less compact method for calculating the area mutually underlying an arbitrary number of circular shadows on the surface of a sphere. Details will be provided to any interested readers.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.