A time-reversing array (TRA) has the ability to retrofocus acoustic energy,
in both time and space, to the original sound-source location without any
information about the acoustic environment in which it is deployed. This un
ique capability may be limited or lost when the acoustic medium or its boun
daries are time dependent, or propagation losses are prevalent. In this pap
er, predictions are made for the size, field-amplitude decay rate (or time)
, and location of the retrofocus for a TRA deployed in the presence of thre
e dynamic acoustic propagation complexities commonly present in shallow oce
an waters: (i) volume scattering from a random superposition of linear inte
rnal waves convecting a gradient in the sound speed profile; (ii) reflectio
n and volume scattering from a deterministic soliton internal wave travelin
g on the thermocline between two water masses with differing sound speed; a
nd (iii) surface scattering from a wind-driven dynamic random rough ocean s
urface. Analytical propagation models for narrow-band signals are used to h
ighlight separately the influence of each propagation complexity on TRA ret
rofocusing. As expected, internal wave time scales are long enough so that
TRA retrofocusing should persist for several minutes for source-array range
s of several kilometers at frequencies approaching 1 kHz. However, the comp
aratively rapid motion of ocean surface waves should prevent TRA exploitati
on of acoustic scattering from a wind-driven ocean surface at ranges greate
r than a few hundred meters, independent of acoustic frequency. Interesting
ly, multiple time-invariant propagation paths are not found to consistently
enhance retrofocusing unless the TRA has sufficient angular resolution to
distinguish them. (C) 1998 Acoustical Society of America. [S0001-4966(98)04
712-2].