diff options
Diffstat (limited to 'desiredata/doc/3.audio.examples/H06.envelope.follower.pd')
-rw-r--r-- | desiredata/doc/3.audio.examples/H06.envelope.follower.pd | 86 |
1 files changed, 0 insertions, 86 deletions
diff --git a/desiredata/doc/3.audio.examples/H06.envelope.follower.pd b/desiredata/doc/3.audio.examples/H06.envelope.follower.pd deleted file mode 100644 index 8f536fba..00000000 --- a/desiredata/doc/3.audio.examples/H06.envelope.follower.pd +++ /dev/null @@ -1,86 +0,0 @@ -#N canvas 87 74 585 621 12; -#X floatatom 354 464 4 0 0 0 - - -; -#X floatatom 150 316 3 0 999 0 - #0-osc2 -; -#X obj 150 336 osc~; -#X text 162 12 ENVELOPE FOLLOWER; -#X text 22 33 An envelope follower measures the mean square power of -an signal as it changes over time. (You can convert mean square power -to RMS ampitude or to decibels if you wish.) The term "mean square" -means simply that the signal should be squared \, and then averaged. -The averageing is done using a low-pass filter such as lop~.; -#X obj 62 466 lop~; -#X floatatom 93 444 3 0 100 0 - #0-lop -; -#X obj 61 356 +~; -#X text 187 317 <-- frequency of second oscillator; -#X obj 62 330 osc~ 500; -#X obj 62 413 *~; -#X obj 62 522 snapshot~; -#X floatatom 62 573 5 0 999 0 - - -; -#X obj 62 545 sqrt; -#X text 335 361 built-in envelope; -#X obj 354 491 dbtorms; -#X floatatom 354 518 5 0 999 0 - - -; -#N canvas 536 459 382 265 startup 0; -#X obj 22 24 loadbang; -#X obj 22 48 bng 15 250 50 0 empty empty empty 0 -6 0 8 -262144 -1 --1; -#X obj 22 67 f \$0; -#X text 35 195 This subpatch loads initial; -#X text 31 219 values in number boxes.; -#X msg 22 91 \; \$1-osc2 400 \; \$1-lop 10 \; \$1-metro 1 \; pd dsp -1; -#X obj 223 132 metro 250; -#X obj 223 107 r \$0-metro; -#X obj 223 156 s \$0-tick; -#X connect 0 0 1 0; -#X connect 1 0 2 0; -#X connect 2 0 5 0; -#X connect 6 0 8 0; -#X connect 7 0 6 0; -#X restore 217 598 pd startup; -#X text 115 414 square the signal; -#X text 124 440 <-- responsiveness; -#X text 159 501 take snapshot; -#X text 108 548 convert to RMS; -#X text 327 599 updated for Pd version 0.39; -#X text 334 381 follower for comparison; -#X text 107 466 low-pass filter; -#X text 114 573 output; -#X obj 70 497 r \$0-tick; -#X text 159 517 every 1/4 second; -#X obj 389 439 r \$0-tick; -#X obj 354 439 f; -#X obj 376 414 env~; -#X text 20 242 The env~ object at right \, which is a built-in envelope -follower using a higher-quality low-pass filter than lop~ \, is shown -for comparison. Its output is artificially slowed down to match the -homemade one at left.; -#X obj 150 359 *~; -#X obj 185 360 tgl 15 0 empty empty empty 0 -6 0 8 -262144 -1 -1 0 -1; -#X text 204 358 <-- on/off; -#X text 20 128 Here we're adding two oscillators so the result should -be an RMS of one if the second oscillator is on \, 0.707 otherwise. -Note two effects: first \, the more responsive the envelope follower -\, the less accurate the result (but the faster it responds). Second -\, if the two oscillators are tuned close to each other their beating -affects the nombers coming out.; -#X connect 0 0 15 0; -#X connect 1 0 2 0; -#X connect 2 0 32 0; -#X connect 5 0 11 0; -#X connect 6 0 5 1; -#X connect 7 0 10 0; -#X connect 7 0 10 1; -#X connect 7 0 30 0; -#X connect 9 0 7 0; -#X connect 10 0 5 0; -#X connect 11 0 13 0; -#X connect 13 0 12 0; -#X connect 15 0 16 0; -#X connect 26 0 11 0; -#X connect 28 0 29 0; -#X connect 29 0 0 0; -#X connect 30 0 29 1; -#X connect 32 0 7 1; -#X connect 33 0 32 1; |