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#X obj 142 443 cos~;
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#X restore 609 405 graph;
#X obj 410 371 pack 0 50;
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#X obj 202 342 -~ 0.5;
#X obj 142 391 *~;
#X obj 410 348 / 10;
#X obj 142 416 clip~ -0.5 0.5;
#X text 408 306 bandwidth;
#X obj 410 417 +~ 1;
#X obj 142 466 +~ 1;
#X obj 283 472 cos~;
#X obj 142 528 *~;
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#X obj 301 337 / 10;
#X text 609 538 --- 0.02 seconds ---;
#X obj 283 446 *~;
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#X obj 563 57 inlet;
#X obj 68 124 tabwrite~ pulse-output;
#X obj 246 57 inlet~;
#X obj 398 57 inlet~;
#X obj 246 124 tabwrite~ window;
#X obj 398 124 tabwrite~ carrier;
#X msg 563 121 \; pd dsp 1;
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#X text 62 15 WINDOWED PACKETS;
#X text 90 480 window;
#X text 318 450 magnified phase;
#X text 73 47 The simpler of two techniques for making slidable center
frequencies is to synthesize enveloped sinusoidal wave packets. The
packets should repeat at the fundamental frequency \, but the frequency
of the packet itself controls the center frequency of the formant.
The length of the packet varies inversely with bandwidth., f 68;
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-1;
#X text 617 623 updated for Pd version 0.37;
#X obj 142 489 *~ 0.5;
#X text 813 180 -1;
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#X text 813 353 -1;
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#X text 814 524 -1;
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#X text 74 135 In the patch below \, the "clip~" followed by "cos~"
and "+~ 1" is the enveloping ("windowing") function \, which appears
in the top graph. The carrier \, on the other hand \, is a broken sinusoid
made by amplifying the phasor~ (the "*~" controlled by "center freq.")
and taking the cos~ of the result. The "breaks" in the sinusoid only
occur when the enveloping signal is zero., f 68;
#X text 90 451 raised;
#X text 90 466 cosine;
#X text 186 252 fundamental frequency, f 11;
#X text 322 473 <= this cosine goes at the;
#X text 323 538 <= graph;
#X text 344 486 desired center frequency but its phase is reset each
fundamental period., f 24;
#X text 289 263 center freq. (in tenths of fundamental), f 13;
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