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New aspects of pseudostationary polymerization and their application
Author(s) -
Olaj Oskar Friedrich,
Zifferer Gerhard
Publication year - 1996
Publication title -
macromolecular symposia
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.257
H-Index - 76
eISSN - 1521-3900
pISSN - 1022-1360
DOI - 10.1002/masy.19961110120
Subject(s) - moment (physics) , polymerization , constant (computer programming) , chain (unit) , analogy , generality , thermodynamics , chemistry , reaction rate constant , state (computer science) , physics , statistical physics , quantum mechanics , kinetics , nuclear magnetic resonance , mathematics , polymer , psychology , linguistics , philosophy , algorithm , computer science , psychotherapist , programming language
Contrary to the stationary state little thought has been given so far to the general principles of the pseudostationary state. In this discourse an attempt is made to demonstrate that — within wide limits — arbitrary initiation profiles may be used to determine k p / k t ( k p = rate constant of chain propagation, k t = rate constant of chain termination) from the frequency dependence of rate of polymerization (in analogy to the rotating‐sector technique) as well as to evaluate k p from the chain‐length distribution (CLD) of samples prepared under pseudostationary conditions. Adverse factors like nonspontaneous transformation of absorbed photons into primary radicals do not invalidate this result. The existence of a universal relationship (independent of the initiation profile) is proved to exist for the second moment of the CLD of samples prepared under pseudostationary initiation conditions for constant (chain‐length independent) k t . Pseudostationarity, however, might be also achieved if not the initiation but the termination is periodically varied. In this case the CLD has a completely different shape but allows determination of k p likewise. Finally, the case of chain‐length dependent k t is shortly discussed in connection with pulsed‐laser initiation. Although the general equation for the second moment of the CLD does not apply any longer for this case some generality appears to exist under these conditions, too.