The cyclization equilibria constant K x is evaluated for the formation of cyclic poly(ethylene terephthalate)s (PET) in the range of degree of polymerization 2 ≤ x ≤ 10 on the basis of an elaborated form of the Jacobson‐Stockmayer theory. According to this theory, K x = W( 0 )·2Γ 0 (1)/(σ cx N A ), where W( r ) is the probability density function for the chain vector r ; Γ 0 (γ) is the probability distribution, when r = 0 of γ = cos Δθ; Δθ being the deviation of the bond angle formed by cyclization from its unconstrained value; σ cx corresponds to the symmetry number of the ring; N A is Avogadro's number. The evaluation of W( r ) is performed in different approximations. The required configurational averages for computing the density distribution W( r ) and the angular correlation factor Γ 0 (1) are obtained by Monte Carlo techniques. The density W ( 0 ) of chain vectors at r = 0 is overestimated by the Gaussian approximation. Values of W( 0 ) calculated in higher approximation lower K x for x < 10. By taking into account the oriental correlation between terminal bonds of the x ‐meric acyclic sequence, K x is lowered additionally by factors of ca. 2,2, 1,3 and 1,1 for x = 4, 5 and 6, respectively. Similar to other polymer chains treated so far, K x is lowered for medium sized chain lengths by taking into account the deviation from Gaussian distribution and angular correlations of chain ends. This result is in contradiction to experimental data, which yield even higher K x ‐values than expected by the classical Jacobson‐Stockmayer theory for medium sized chain lengths. The inclusion of cis ‐ester residues into the all trans ‐ester PET chain only slightly reduces this discrepancy. Structural modifications of the PET chain during cyclization experiments are discussed as a rationale for the deviations from the present theory.
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Suter et al. (1979) studied this question.
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