It has recently been found that the heat transfer in the vicinity of t
he liquid-vapor critical point is governed by a fourth heat transfer p
rocess called Piston Effect. This effect has been described as the str
ong expansion of a thin initial thermal boundary layer (due to the div
erging compressibility of near-critical fluids), driving in the rest o
f the fluid a set of compression waves which adiabatically increase th
e temperature, on a shorter and shorter time-scale as the critical poi
nt is approached (Critical Speeding Up). In the present work, matched
asymptotic descriptions techniques applied to the Navier-Stokes equati
ons show that very near the critical point, a new regime of heat trans
fer appears where thermal equilibration is governed only by acoustic p
henomena. In this new regime, temperature relaxation takes place withi
n a few acoustic typical times only, showing that the Piston-Effect me
chanism can be as fast as the acoustic propagation, but no faster. Thi
s phenomenon is called the Acoustic Saturation of the Piston Effect.