Abstract
The distribution of cyclic species is explored for an irreversible Ag-R-Bf-g model on the basis of the concept of the “m tree” which was introduced in a preceding report by the authors. On the assumption of equal reactivity, the explicit solution is derived; i.e., for a sufficiently concentrated solution the concentration of cyclicj-mers can be expressed as\(\left[ {R_j } \right] = \left( {k_{Rj} /k_L } \right)\left[ {\left( {f - g} \right)D_B } \right]^j \omega _j /j\), wherek Rj andk L are the rate constants of cyclicj-mer formation and interconnection, respectively, and
where α=(g − 1)(f − g − 1)/g(f − g) and [j/2] is the Gauss' symbol. Forg → 1, ωj → 1, so that the solution reduces to the A-R-Bf−1 case. At a critical point one observes the strong divergence of the chances ∑ φj of cyclization.
References
P. J. Flory,J. Am. Chem. Soc. 63:3083 (1941).
W. H. Stockmayer,J. Chem. Phys. 11:45 (1943).
M. Gordon,Proc. R. Soc. A 268:240 (1962).
W. Burchard,Adv. Polymer Sci. 48:1 (1983).
S. I. Kuchanov, S. V. Korolev, and S. V. Panyukov,Adv. Chem. Phys. 43:115 (1988).
C. W. Macosko and D. R. Miller,Macromolecules 9:199 (1976).
P. G. de Gennes,Scaling Concept in Polymer Physics (Cornell University Press, Ithaca, New York, 1979), Chapter V.
D. Stauffer, A. Coniglio, and M. Adam,Adv. Polymer Sci. 44:103 (1982).
K. Suematsu and T. Okamoto,J. Stat. Phys., to appear.
W. Kühn,Kolloid Z. 68:2 (1934).
H. Jacobson and W. H. Stockmayer,J. Chem. Phys. 18:1600 (1950).
J. L. Spouge,J. Stat. Phys. 43:143 (1986);Macromolecules 16:121 (1983).
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Suematsu, K., Okamoto, T. Distribution of cyclic species in network formation: Microscopic theory of branching process in Ag-R-B f−g model. J Stat Phys 66, 661–668 (1992). https://doi.org/10.1007/BF01060087
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DOI: https://doi.org/10.1007/BF01060087