ZntroductionSeveial reports have been published concerning the discontinuities of the physical and dynamic properties of poly(ethy1ene glycol) (PEG) with an average molecular weight range of R,S 1OOOO. Thus, spin-labelling relaxation measurements revealed an anomalously high activation energy value in the melting region of PEG with M,=1550'. Surface tension (y) measurements of PEG as a function of molecular weight (M,) gave a minimum y-value at My= 1300 (T=353 K)2. Also the viscoelastic behaviour of PEG is anomalous in the R, range of -20003. These results have been explained in terms of the onset of chain f~l d i n g~-~ and of the end group effect7.'The use of proton decoupled carbon-13 nuclear magnetic resonance spectra ( 13C-{ 'H}NMR) in the elucidation of PEG and PEG-maleic anhydride copolymer microstructures is documented *. Our earlier studies of PEG dynamics by spin-labelling technique were concentrated nearest upon the end group and interphase effects 1*7. By means of carbon-I3 relaxation measurements it is also possible to get infdrmation about the backbone dynamics of PEG chains. Therefore we have studied the change of carbon-13 spin lattice relaxation times (TI) of PEG melts as a function of R, (R,=600-20000) to get a clearer view about the PEG chain dynamics in this molecular weight region.