| Eli Brandt wrote:
>As a first approximation, think of "tone" as having no effect below
>the cutoff frequency, and attenuating above it. The amount of
>attenuation is proportional to how many *octaves* the signal is above
>the cutoff. (6 dB/octave for a one-pole filter, specifically.)
>
>But 0 Hz is at minus infinity on the octave scale. If you pick this
>as the cutoff, nothing will get through. (Except DC, and in practice
>that probably won't work either.)
This works well. However, plugging a bunch of different values into khp
for tone and atone suggests that the amplitude response curves of tone and
atone look something like these (which raise some questions):
AMPLITUDE RESPONSE CURVE OF TONE
|
|
|
ouput |
amp | /-------------\ <-------- just below input amp value (90-97%)
values | / \
| / \ N.B. the plateau isn't really flat;
| / \ the slope of the rise gradually decreases
|/ \
-------------------------
0 sr/2 sr
Question:
(1) Why doesn't tone's passband allow the input signal to pass at 100%
power? (With a noise input of 10000, the maximum output signal amp is
~9700).
AMPLITUDE RESPONSE CURVE OF ATONE
|
|
| /\ /\ |-------- these output amps are *greater*
ouput |/ \ / \ |-------- than the input amp!
amp | -- -- <-------- input amp value
values | -- --
| -- --
| ------
|
---------------------------
0 sr/2 sr
Questions:
(1) How is it possible that an output signal from atone can have a greater
amplitude than the input signal? (When sr = 10000 and noise with an amp of
10000 is filtered with khp = 400, the output amp is ~12100).
(2) Why does the output signal amp constantly decrease as khp -> sr/2?
Shouldn't the passband that is *not* filtered out output at 100% of the
input power? (When sr = 10000 and noise with an amp of 10000 is filtered
with khp = 2500, the output signal is only 5000 rather than 10000).
Trevor Baca
tbaca@ccwf.cc.utexas.edu
|