Frequency resolving power (FRP) of the human's hearing was measured us
ing the rippled noise as a probe. To examine the ripple discrimination
, a phase-reversal test was used: the rippled noise was replaced by th
at with the opposite peak and through positions. This switch can be de
tected only when rippled structure of the noise spectrum is discrimina
ted. The highest ripple density when the switch was detectable was tak
en as a FRP measure. Narrow-band rippled spectra were used to measure
the FRP within a frequency range of 0.175 to 11 kHz. The highest resol
vable ripple density in absolute measure (ripples number per kHz) was
about 21/kHz at frequencies below 0.5 kHz and fell down at higher freq
uencies. Resolvable ripple density in relative measure (central freque
ncy divided by ripple spacing) was about 22 relative units at frequenc
ies above 2.8 kHz and fell down al lower frequencies.