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#X text 523 433 ---- 0.02 seconds ----;
#X text 542 501 updated for Pd version 0.37;
#X text 445 210 0;
#X text 484 229 -- partial number --;
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#X text 708 74 0.5;
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#X text 57 23 This is a modified version of the pulse train generator from two examples back.;
#X text 56 72 We have to add 1/2 and wrap so that the center of the pulse comes at phase zero (previously it was 1/2 cycle out of phase). This wasn't a problem before but now we have to be in phase with the oscillator we're multiplying with.;
#X text 262 160 otherwise it's the same as before.;
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#X text 171 140 multiple of fundamental;
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#X text 93 93 Fourier series;
#X text 98 146 magnitude;
#X text 96 131 calculate;
#X text 21 3 This subpatch computes the spectrum of the incoming signal with a (rectangular windowed) FFT. FFTs aren't properly introduced until much later.;
#X text 83 61 signal to analyze;
#X text 193 164 delay two samples;
#X text 191 182 for better graphing;
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#X text 298 231 toggle to graph repeatedly;
#X text 262 212 bang to graph once;
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#X obj 19 295 tabwrite~ F05-signal;
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#X msg 224 321 \; pd dsp 1;
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#X text 156 196 modulating oscillator;
#X text 64 16 RING MODULATED PULSE TRAINS;
#X text 69 371 Now we take a pulse train and ring modulate it \, which effectively aliases the spectrum so that it is centered at any desired partial number. The "bandwidth" control still affects the shape of the peak \, independently of where it is centered. This generates a formant centered at the given partial., f 55;
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#X text 69 467 This patch is limited to making formants centered on harmonics. The center frequency thus can't be moved smoothly up and down at will (try shift-clicking on modulation frequency to make fractions). Next we'll look at two techniques for sliding a formant frequency without losing harmonicity., f 55;
#X text 201 97 generator from before;
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#X text 188 228 <-- graph once;
#X text 228 253 <-- repeatedly;
#X text 124 57 <-- bandwidth;
#X text 202 81 <-- pulse train;
#X text 143 126 <-- modulation frequency as;
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