We re-examine the problem of the diffusion of a Gaussian chain in a fixed a
rray of obstacles using the projection operator formalism introduced by Lor
ing [J. Chem. Phys. 88, 6631 (1988)]. We show that in the limit of long wav
elengths, the frequency-dependent monomer friction coefficient that is used
in the calculation of the mean square displacement of the center of mass c
an be rewritten exactly in terms of the time correlation function of the to
tal force on the chain. When the decay profile of the force correlation fun
ction is assumed to be exponential, and its dependence on the density of ob
stacles written in an approximate resummed form, the dynamics of the center
of mass is found to be diffusive at long and short times, and subdiffusive
(anomalous) at intermediate times. Moreover, the diffusion coefficient D t
hat describes the long-time behavior of the chain at high concentrations of
small obstacles is found to vary with chain length N as N-2, which is in q
ualitative agreement with the predictions of the reptation model. These res
ults are obtained in the absence of any mechanism that might incorporate th
e notion of reptation directly into the calculations, in contrast to Loring
's approach, which treats the monomer friction coefficient approximately us
ing a decoupling of segmental motion into parallel and perpendicular compon
ents. (C) 2000 American Institute of Physics. [S0021-9606(99)50747-2].