Abstract
The enumeration theory is extended in this work into a more general theory, taking back-reactions into consideration. The solutions may faithfully reproduce real processes from arbitrary starting points to a steady-state. Therefore, the presented theory includes the equilibrium theory by Jacobson-Stockmayer, the numerical solution by Gordon-Temple, and the irreversible theory by the present authors. The solutions are described first in general forms of transition probabilities {P}, and then explicitly with the aid of rate equations; simple proofs are given. The presented theory was applied to an experimental data: the distribution of cyclic species in poly(ethylene terephthalate). We shall show that agreement between theory and experiment is nearly perfect.
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Abbreviations
- N 0 :
-
Total number of units
- V :
-
System volume
- C 0=N 0/N A ·V :
-
Initial concentration (N A : Avogadro's number)
- L x :
-
AB type chain x-mer; (AB)x
- N x :
-
Number of AB type x-mers
- R x :
-
Ring x-mer
- N Rx :
-
Number of ring x-mers
- E :
-
Small molecule eliminated by bond-formation
- N E :
-
Number of small molecules eliminated by bond-formation
- h k :
-
Number of reacted functional units (f.u.) in statek
- ξ k :
-
Number of reacted functional units (f.u.) in chains in statek
- Ξ k :
-
Total number of units in chains in statek
- D=h k /N 0 :
-
Extent of reaction in statek
- D *=ξ k /Ξ k :
-
Extent of reaction in chains in statek
- k L :
-
Chain-propagation rate constant
- k Rx :
-
Cyclization rate constant of chain x-mers
- k B :
-
Bond breakage rate constant of chains
- k B,Rx :
-
Bond breakage rate constant of cyclic x-mers
- <k Rx > k :
-
Mean cyclization rate constant in statek
- g(x)=k B,Rx /k B :
-
Ring-opening factor of cyclic x-mers
- P Lx,k :
-
Probability that a chain x-mer will be formed in statek
- {P}:
-
Set of transition probabilities per single jump in forward direction or reverse direction (see the text on individual transition probabilities)
- M A :
-
Total AA monomer unit number
- M B :
-
Total BB monomer unit number
- M 0=M A +M B :
-
Total particle number
- ζ A,i =2M A −h i :
-
Unreacted A functional unit (f.u.) number in statei
- ζ B,i =2M B −h i :
-
Unreacted B f.u. number in statei
- ζ Ax :
-
Unreacted A f.u. number on x-mers
- h i :
-
Number of reacted A (or B) f.u. in statei
- ξ i :
-
Number of reacted A (or B) f.u. in chains in statei
- Ξ A,i =2M A −h i +ξ i :
-
A f.u. number in chains in statei
- Ξ B,i =2M B −h i +ξ i :
-
B f.u. number in chains in statei
- Ξ i =2(M 0−h i +ξ i ):
-
Total f.u. number in chains in statei
- D=h i /M 0 :
-
Extent of reaction in statei
- D * A =ξ i /Ξ A,i :
-
Extent of reaction of A f.u. in chains in statei
- D * B =ξ i /Ξ B,i :
-
Extent of reaction of B f.u. in chains in statei
- D *=2ξ i /Ξ i :
-
Extent of reaction in chains in statei
- L αx :
-
(AA-BB)x-1-AA type chain x-mer;x=1,2,3,...
- L βx :
-
BB-(AA-BB)x type chain x-mer;x=0,1,2,...
- L γx :
-
(AA-BB)x type chain x-mer;x=1,2,3,...
- N αx :
-
Number of α type x-mers
- N βx :
-
Number of β type x-mers
- N γx :
-
Number of γ type x-mers
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Suematsu, K., Okamoto, T. Theory of ring formation in a reversible system: general solutions. Colloid Polym Sci 270, 405–420 (1992). https://doi.org/10.1007/BF00665983
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DOI: https://doi.org/10.1007/BF00665983