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Volumn 2, Issue 3, 1998, Pages 341-345

The effect of added salt on polyelectrolyte structure

Author keywords

30.20.Ey Conformation (statistics and dynamics); 61.25.Hq Macromolecular and polymer solutions; polymers melts; swelling; 87.15.He Molecular dynamics and conformational changes

Indexed keywords

COMPOSITION EFFECTS; COMPUTER SIMULATION; CONDENSATION; CONFORMATIONS; MACROMOLECULES; MOLECULAR DYNAMICS; MOLECULAR STRUCTURE; SODIUM CHLORIDE; SOLUTIONS; SWELLING;

EID: 0031680502     PISSN: 14346028     EISSN: None     Source Type: Journal    
DOI: 10.1007/s100510050257     Document Type: Article
Times cited : (70)

References (24)
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    • U. Micka, K. Kremer, Phys. Rev. E54, 2653 (1996); Europhys. Lett. 38, 279 (1997).
    • (1997) Europhys. Lett. , vol.38 , pp. 279
  • 7
  • 8
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    • M. Stevens, K. Kremer, Macromol. 26, 4717 (1993); Phys. Rev. Lett. 71, 2228 (1993).
    • (1993) Phys. Rev. Lett. , vol.71 , pp. 2228
  • 9
    • 0017468271 scopus 로고
    • T. Odijk, J. Polym. Sci. Polym. Phys. Ed. 15, 477 (1977); J. Skolnick, M. Fixman, Macromol. 10, 944 (1977); J.-L. Barrat, J.-F. Joanny, Europhys. Lett. 3, 343 (1993).
    • (1977) J. Polym. Sci. Polym. Phys. Ed. , vol.15 , pp. 477
    • Odijk, T.1
  • 10
    • 4243189532 scopus 로고
    • T. Odijk, J. Polym. Sci. Polym. Phys. Ed. 15, 477 (1977); J. Skolnick, M. Fixman, Macromol. 10, 944 (1977); J.-L. Barrat, J.-F. Joanny, Europhys. Lett. 3, 343 (1993).
    • (1977) Macromol. , vol.10 , pp. 944
    • Skolnick, J.1    Fixman, M.2
  • 11
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    • T. Odijk, J. Polym. Sci. Polym. Phys. Ed. 15, 477 (1977); J. Skolnick, M. Fixman, Macromol. 10, 944 (1977); J.-L. Barrat, J.-F. Joanny, Europhys. Lett. 3, 343 (1993).
    • (1993) Europhys. Lett. , vol.3 , pp. 343
    • Barrat, J.-L.1    Joanny, J.-F.2
  • 19
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    • For salt-free systems, some quantities are not as accurately calculated in the DH approximation, see M. Stevens, K. Kremer, J. Phys. I France 6, 1607 (1996).
    • (1996) J. Phys. I France , vol.6 , pp. 1607
    • Stevens, M.1    Kremer, K.2
  • 21
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    • For sufficiently large λ, the exponential screening dominates, but as in this case such large values tend to be unphysical
    • For sufficiently large λ, the exponential screening dominates, but as in this case such large values tend to be unphysical.


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