Jh. Jang et al., A Monte Carlo simulation on the effects of chain end modification on freely standing thin films of amorphous polyethylene melts, MACROMOLEC, 33(20), 2000, pp. 7663-7671
The effects of chain end modification on freely standing amorphous polyethy
lene thin films with a thickness 2R(g) to 4R(g) (radius of gyration) are st
udied by a Monte Carlo (MC) simulation on a high coordination lattice. The
rotational isomeric state (RIS) model is incorporated into the simulation a
s short-range interactions, and a Lennard-Jones (LJ) potential is used to c
alculate the long-range interactions. The modification of the chain ends is
introduced by changing the well-depth (epsilon) of the LJ potential as com
pared to the middle beads. Chain ends with epsilon(end) less than or equal
to epsilon(middle) show segregation near the free surface, but chain ends w
ith epsilon(end) much greater than epsilon(middle) prefer to remain in the
bulklike region. Both entropy and enthalpy are major factors in the determi
nation of the distribution of the chain ends. The effects of the free surfa
ce can extend farther than R-g into the interior of the thin film. However,
for the case of relatively attractive chain end (epsilon(end) slightly lar
ger than epsilon(middle)), a fairly large length of isotropic region is obs
erved at the molecular level due to the balance of the entropic effect to p
refer a free surface and the enthalpic effect to prefer bulk region. The re
pulsive chain ends (epsilon(end) < epsilon(middle)) induce faster dynamics
in the middle region of the film as observed by the center-of-mass displace
ment and the chain shape autocorrelation function.