Scattering activities and symmetry of skeletal stretching vibrations of long chain molecules by Raman spectroscopy

1983 ◽  
Vol 78 (7) ◽  
pp. 4777-4779 ◽  
Author(s):  
M. Harrand
Keyword(s):  
Raman Spectroscopy ◽  
Chain Molecules ◽  
Stretching Vibrations ◽  
Long Chain

Change of Damping for Long-Chain Molecules during Solidification and Melting in Scattering Samples Studied by Raman Spectroscopy

2008 ◽  
Vol 47 (10) ◽  
pp. 7936-7940
Author(s):  
Kazi Monowar Abedin ◽  
Jun-ichi Shikata ◽  
Katsuhiko Miyamoto ◽  
Hiromasa Ito
Keyword(s):  
Raman Spectroscopy ◽  
Chain Molecules ◽  
Long Chain

scholarly journals The Excluded Volume Effect of Very-long-chain Molecules

1968 ◽  
Vol 41 (2) ◽  
pp. 538-538 ◽  
Author(s):  
Keizo Suzuki
Keyword(s):  
Volume Effect ◽  
Excluded Volume ◽  
Chain Molecules ◽  
Excluded Volume Effect ◽  
Long Chain

Velocity autocorrelation function for the motion of long-chain molecules in the free draining limit

1973 ◽  
Vol 8 (4) ◽  
pp. 367-371
Author(s):  
B. Caroli ◽  
G. Jannink ◽  
D. Saint-James ◽  
D. Taupin
Keyword(s):  
Autocorrelation Function ◽  
Velocity Autocorrelation Function ◽  
Chain Molecules ◽  
Velocity Autocorrelation ◽  
Long Chain

Effect of density on configurational properties of long-chain molecules using a Monte Carlo method

1966 ◽  
Vol 62 ◽  
pp. 3319 ◽  
Author(s):  
S. G. Whittington ◽  
D. Chapman
Keyword(s):  
Monte Carlo ◽  
Monte Carlo Method ◽  
Chain Molecules ◽  
Long Chain

Conformational transitions of long chain molecules in frozen solutions

1989 ◽  
Vol 91 (11) ◽  
pp. 7296-7299 ◽  
Author(s):  
R. Hirschmann ◽  
J. Friedrich ◽  
E. Daltrozzo
Keyword(s):  
Conformational Transitions ◽  
Chain Molecules ◽  
Frozen Solutions ◽  
Long Chain

Theory of Depolymerization of Long Chain Molecules

1940 ◽  
Vol 8 (9) ◽  
pp. 721-726 ◽  
Author(s):  
Elliott W. Montroll ◽  
Robert Simha
Keyword(s):  
Chain Molecules ◽  
Long Chain

Intrinsic viscosities and unperturbed dimensions of long chain molecules

2006 ◽  
pp. 196-312 ◽  
Author(s):  
Michio Kurata ◽  
Walter H. Stockmayer
Keyword(s):  
Chain Molecules ◽  
Unperturbed Dimensions ◽  
Long Chain

The Nucleation of Long-Chain Molecules in Monomolecular Layers1

1965 ◽  
Vol 69 (3) ◽  
pp. 956-959 ◽  
Author(s):  
L. Mandelkern ◽  
J. G. Fatou ◽  
C. Howard
Keyword(s):  
Chain Molecules ◽  
Long Chain

The diffusion of long-chain molecules through bulk polyethelene

1979 ◽  
Vol 365 (1720) ◽  
pp. 53-73 ◽  
Keyword(s):  
Polymer Melt ◽  
Appreciable Effect ◽  
Interfacial Resistance ◽  
Chain Molecules ◽  
Surface Migration ◽  
The Matrix ◽  
Activation Energy For Diffusion ◽  
Matrix Morphology ◽  
Entangled Polymer ◽  
Long Chain

This paper describes an experimental study of the centre of mass diffusion of linear hydrocarbon or deuterocarbon molecules, of the type (CH 2 ) N or (CD 2 ) N , through bulk polyethylene. N was varied between about 15 and 1500. The diffusion coefficient D was measured as a function of temperature, matrix morphology and diflfusant chain length, both in semi-crystalline and molten polyethylene. The technique used involved labelling the diflfusants so that they absorbed radiation in the infrared spectrum in a region relatively free of absorption by the matrix. Infrared microdensitometry was used to measure diffusion broadening of a known diffusant concentration distribution, and hence to evaluate D . The method avoids problems presented by interfacial resistance and surface migration effects and can also account for the effect of diffusant polydispersity. The diffusion was found to be Fickian and essentially independent of concentration, for the diflfusants used, up to 2%. The data indicate that the morphology of the disordered interlamellar region can have an appreciable effect on the mobility of long-chain diffusants. They also suggest that the activation energy for diffusion in the melt becomes independent of diflfusant length beyond a certain lower limit. The results provide support for de Gennes’s (1971) model of snake-like motion (reptation) for polymeric diflfusants in an entangled polymer melt, and suggest that such motion persists down to a diflfusant size of some 30-(CH 2 )-backbone units.

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