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Concentration dependence of the global and anisotropic dimensions of confined macromolecules
Author(s) -
Cifra Peter,
Bleha Tomáš
Publication year - 2000
Publication title -
macromolecular theory and simulations
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.37
H-Index - 56
eISSN - 1521-3919
pISSN - 1022-1344
DOI - 10.1002/1521-3919(20001101)9:8<555::aid-mats555>3.0.co;2-z
Subject(s) - anisotropy , perpendicular , scaling , polymer , chain (unit) , distribution function , condensed matter physics , materials science , macromolecule , molecular physics , chemistry , physics , optics , geometry , composite material , thermodynamics , quantum mechanics , mathematics , biochemistry
The chain dimensions 〈 R 2 〉 of nondilute polymer solutions confined to a slit of the width D were studied using lattice simulations. It was found that the chain compression induced in good solvents by the concentration ϕ is enhanced in a slit relative to the bulk. The global dimensions of chains also change with ϕ in confined and unconfined theta solutions. At intermediate slit widths, a region was noted where coils are squeezed along all three axes. This region is manifested as a channel on the three‐dimensional surface 〈 R 2 〉( D ,ϕ) in both good and theta solvents. The coil anisotropy, given by the ratio of the parallel and perpendicular components of the chain dimensions 〈 R y 2 〉/〈 R x 2 〉, reaches high values at strong confinements, where coils form quasi‐two‐dimensional pancakes. The concentration‐induced reduction of the global chain dimensions in good solvents is almost fully transmitted to the parallel component 〈 R y 2 〉. The computed effects of concentration and confinement were compared with the predictions of mean‐field and scaling theories, and implications of the results to ultrathin films and layered nanocomposites were discussed. In addition, the distribution functions of the components of the end‐to‐end distance R perpendicular and parallel to the plates, W ( R x ) and W ( R y ), were calculated. The function W ( R x ) combined with the concentration profile ϕ ( x ) along the pore provided details of the chain structure close to walls. A marked difference in the pace of the filling up of the depletion layer was noticed between chains in theta and good solvents. From the distribution functions W ( R x ) and W ( R y ), the highly anisotropic force‐elongation relations imply the deformation of chains in confined solutions and ultrathin bulk films.