Multiscale asymptotic methods developed previously to study macromechanical wave propagation in cochlear models are generalized here to include active control of a cochlear partition having three subpartitions, the basilar membrane, the reticular lamina, and the tectorial membrane. Activation of outer hair cells by stereocilia displacement and/or by lateral wall stretching result in a frequencydependent force acting between the reticular lamina and basilar membrane. Wavelength-dependent fluid loads are estimated by using the unsteady Stokes' equations, except in the narrow gap between the tectorial membrane and reticular lamina, where lubrication theory is appropriate. The local wavenumber and subpartition amplitude ratios are determined from the zeroth order equations of motion. A solvability relation for the first order equations of motion determines the subpartition amplitudes. The main findings are as follows: The reticular lamina and tectorial membrane move in unison with essentially no squeezing of the gap; an active force level consistent with measurements on isolated outer hair cells can provide a 35-dB amplification and sharpening of subpartition waveforms by delaying dissipation and allowing a greater structural resonance to occur before the wave is cut off; however, previously postulated activity mechanisms for single partition models cannot achieve sharp enough tuning in subpartitioned models.The cochlea consists of a liquid-filled spiral helix channel embedded in the temporal bone. Cross-sections along its axis are divided into two main chambers, the scalae, by a cochlear partition (CP) composed of two parallel fibrous membranes, the basilar membrane (BM) and tectorial membrane (TM) with a complex cell structure between them. A thin gap separates the reticular lamina (RL), which is the upper surface of the cell complex, from the TM (Fig. 1). Both efferent and afferent nerve fibers are attached to the synaptic ends of two particular cell groups, the inner and outer hair cells (IHC and OHC, respectively). These cells derive their names from the bundles of hair-like projections called stereocilia. The stereocilia lie in the thin liquid-filled gap between the RL and TM with the tips of the OHC stereocilia embedded in the TM. Their displacement, caused by the CP motion, modulates both transmembrane and receptor potentials of both cell types. This property allows afferent neurons from the IHCs to carry neural discharges of encoded acoustic signals to the auditory cortex, while the efferent neurons to the OHCs evidently regulate their motility properties. The axial variations of the CP are known to effect spatial frequency filtering of the acoustic wave. Frequency discrimination is directly related to the sharpness of these spatial filters. Impressive frequency response quality factors (Q 10) have been measured for both neural discharges and CP mechanical oscillations. As this sharpness cannot be solely attributed to passive mechanicalThe publication costs of this article were defrayed in part by p...