Wh. Tang et al., THEORY FOR THE NONEQUILIBRIUM DYNAMICS OF FLEXIBLE CHAIN MOLECULES - RELAXATION TO EQUILIBRIUM OF PENTADECANE FROM AN ALL-TRANS CONFORMATION, The Journal of chemical physics, 108(20), 1998, pp. 8736-8742
We extend to nonequilibrium processes our recent theory for the long t
ime dynamics of flexible chain molecules. While the previous theory de
scribes the equilibrium motions for any bond or interatomic separation
in (bio)polymers by time correlation functions, the present extension
of the theory enables the prediction of the nonequilibrium relaxation
that occurs in processes, such as T-jump experiments, where there are
sudden transitions between, for example, different equilibrium states
. As a test of the theory, we consider the ''unfolding'' of pentadecan
e when it is transported from a constrained all-trans conformation to
a random-coil state at thermal equilibrium. The time evolution of the
mean-square end-to-end distance [R-end(2)(t)](noneq) after release of
the constraint is computed both from the theory and from Brownian dyna
mics (BD) simulations. The lack of time translational symmetry for non
equilibrium processes requires that the BD simulations of the relaxati
on of [R-end(2)(t)](noneq) be computed from an average over a huge num
ber of independent trajectories, rather than over successive configura
tions from a single trajectory, which may be used to generate equilibr
ium time correlation functions. Adequate convergence ensues for the no
nequilibrium simulations only after averaging 9000 trajectories, each
of 0.8 ns duration. In contrast, the theory requires only equilibrium
averages for the initial and final states, which may be readily obtain
ed from a few Brownian dynamics trajectories. Therefore, the new metho
d produces enormous savings in computer time. Moreover, since both the
ory and simulations use identical potentials and solvent models, the t
heory contains no adjustable parameters. The predictions of the theory
for the relaxation of [R-end(2)(t)](noneq) agree very well with the B
D simulations. This work is a starting point for the application of th
e new method to nonequilibrium processes with biological importance su
ch as the helix-coil transition and protein folding. (C) 1998 American
Institute of Physics. [S0021-9606(98)50720-9].