TY - JOUR
T1 - RADIATION CHEMISTRY OF LINEAR LOW-DENSITY POLYETHYLENE. II. KINETICS OF ALKYL AND ALLYL FREE-RADICAL DECAY REACTIONS.
AU - Basheer, Rafil
AU - Dole, Malcolm
PY - 1983
Y1 - 1983
N2 - In the reported experiments, quenched and annealed samples of linear low-density polyethylene (LLDPE) were gamma irradiated in vacuo at 77 K; the kinetics of the alkyl free-radical decay reactions were studied at room temperature, and of the allyl free-radical reactions at 60, 70, and 80 degree C. The ESR signals saturate at a slightly higher microwave power in the LLDPE than in high-density polyethylene (HDPE), and the alkyl radicals start decaying at a lower temperature in the LLDPE than in the HDPE. As in the HDPE the decay of the alkyl free radicals at room temperature in the LLDPE follows the kinetic equation for two simultaneous first-order reactions with the fraction of the faster-decaying component being slightly greater in the quenched than in the annealed samples. In the case of the allyl free radicals the decay at 60 degree C follows the equation based on one fraction of the radicals decaying according to second-order kinetics in the presence of other nondecaying radicals. At higher temperatures the data are best understood in terms of a second-order rate equation with a continuously variable time-dependent rate constant as suggested by Hamill and Funabashi.
AB - In the reported experiments, quenched and annealed samples of linear low-density polyethylene (LLDPE) were gamma irradiated in vacuo at 77 K; the kinetics of the alkyl free-radical decay reactions were studied at room temperature, and of the allyl free-radical reactions at 60, 70, and 80 degree C. The ESR signals saturate at a slightly higher microwave power in the LLDPE than in high-density polyethylene (HDPE), and the alkyl radicals start decaying at a lower temperature in the LLDPE than in the HDPE. As in the HDPE the decay of the alkyl free radicals at room temperature in the LLDPE follows the kinetic equation for two simultaneous first-order reactions with the fraction of the faster-decaying component being slightly greater in the quenched than in the annealed samples. In the case of the allyl free radicals the decay at 60 degree C follows the equation based on one fraction of the radicals decaying according to second-order kinetics in the presence of other nondecaying radicals. At higher temperatures the data are best understood in terms of a second-order rate equation with a continuously variable time-dependent rate constant as suggested by Hamill and Funabashi.
UR - http://www.scopus.com/inward/record.url?scp=0020766858&partnerID=8YFLogxK
U2 - 10.1002/pol.1983.180210612
DO - 10.1002/pol.1983.180210612
M3 - Article
AN - SCOPUS:0020766858
SN - 0449-2978
VL - 21
SP - 957
EP - 967
JO - Journal of polymer science. Part A-2, Polymer physics
JF - Journal of polymer science. Part A-2, Polymer physics
IS - 6
ER -