Yn. Kaznessis et al., Dielectric relaxation of dipole-inverted polar polymers as studied by computer simulations, MACROMOLEC, 32(20), 1999, pp. 6679-6686
We use molecular dynamics simulations to examine the dielectric relaxation
of polar macromolecules with dipoles parallel to the chain backbone. Analys
is of the simulation trajectories closely follows the treatment of Watanabe
and co-workers for experimental results of dipole-inverted cis-polyisopren
e solutions (Macromolecules 1995, 28, 6443). The important observable quant
ity in experiments and simulations is the dielectric loss spectrum epsilon
"(omega), whose shape reflects the distribution of relaxation processes for
the global chain motion. The observed broadening of the spectra with incre
asing polymer concentration, classically attributed to overlapping of the c
hains, is analyzed quantitatively using a local correlation function C(n,t;
m) = 1/a(2) [u(n,t).u(m,0)], where u(n,t) is the bond vector of the nth seg
ment of the chain at time t, and a(2) = [u(2)]. At long times, C(n,t;m) can
be expanded as a sum of its eigenmodes: C(n,t;m) = 2/N(n)Sigma(p=1)f(p)(m)
f(p)(m) exp(-t/tau(p)), where N is the size of the chain and tau(p) and f(p
) are the relaxation time and the eigenfunction of the pth mode. From simul
ations we calculate the time correlation functions and dielectric loss spec
tra of multi-inverted and asymmetrically inverted polar polymers. We comput
e the relaxation times tau(p) and the eigenfunctions of C(t,n;m). The relax
ation times follow a power-law dependence tau p proportional to p(-gamma),
with gamma similar or equal to 2.08, and the ratios tau(p)/tau(1) remain in
dependent of the concentration, a behavior predicted by the Rouse model. On
the other hand, the dependence off, on n deviates progressively with incre
asing density from the Rouse model sinusoidal prediction. The results revea
l that the broadening of the spectra is a result of changes in the distribu
tion of eigenmodes (f(p)), and not in the relaxation time span gamma. Our.
findings are consistent with the experimental observations, clearly demonst
rating the adequacy of simulations for investigating the dynamic behavior o
f macromolecular systems.