THE COLLAPSE OF CHAINS WITH DIFFERENT ARCHITECTURES

Citation
G. Raos et al., THE COLLAPSE OF CHAINS WITH DIFFERENT ARCHITECTURES, The Journal of chemical physics, 100(10), 1994, pp. 7804-7813
Citations number
21
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
100
Issue
10
Year of publication
1994
Pages
7804 - 7813
Database
ISI
SICI code
0021-9606(1994)100:10<7804:TCOCWD>2.0.ZU;2-Z
Abstract
The equilibrium properties and the Rouse-Zimm dynamics of polymer mole cules with any architecture at temperatures T less than or equal to Th eta, are treated using a bead-and-spring coarse-grained description. T he collapsed globule model is adopted, whereby essentially all atoms a re at the same mean-square distance (S-2) from the center of mass; acc ordingly, at a given temperature the interatomic free energy is a sing le-valued function of (S-2) and the self-consistent free-energy minimi zation is greatly simplified, in the Gaussian approximation. We prove that the connectivity matrix B and the bond-vector product matrix M=[( I-i.I-j)] possess the same eigenvectors; these are the normal modes of the chain conformation. Furthermore, we show that (S-2)=N(at)(-1)Sigm a(k)l(2) alpha(k)(2)/lambda(k), where N-at is the total number of atom s, lambda(k) is the general nonzero eigenvalue of B, and l(2) alpha(k) (2) is the corresponding eigenvalue of M-the expansion ratio of the no rmal mode. Finally, we prove that in the free-draining limit the norma l mode relaxation times are proportional to l(2) alpha(k)(2)/lambda(k) . Defining as alpha(s)=root(S-2)/(S-2)(ph) as the overall strain ratio with respect to the phantom state, the plots of alpha(s) vs the reduc ed temperature tau=(T-Theta)/T less than or equal to 0 indicate that p olymers with more compact architectures display a prompter contraction for small \tau\'s, although tending to larger alpha(s)'s at strong un dercoolings, where the average density (alpha N-at.(S-2)(-3/2)) is abo ut the same for all architectures. Concerning the dynamical behavior, at sufficiently large \tau\'s the longest relaxation times reach a typ ical plateau, as already found for the linear chain.