From 4d84d14ac1aa13958eaa2971b03f7f929a519105 Mon Sep 17 00:00:00 2001
From: =?UTF-8?q?IOhannes=20m=20zm=C3=B6lnig?=
 <zmoelnig@users.sourceforge.net>
Date: Fri, 8 Feb 2008 13:00:32 +0000
Subject: reorganized

svn path=/trunk/; revision=9400
---
 desiredata/doc/3.audio.examples/E10.complex.FM.pd | 156 ++++++++++++++++++++++
 1 file changed, 156 insertions(+)
 create mode 100644 desiredata/doc/3.audio.examples/E10.complex.FM.pd

(limited to 'desiredata/doc/3.audio.examples/E10.complex.FM.pd')

diff --git a/desiredata/doc/3.audio.examples/E10.complex.FM.pd b/desiredata/doc/3.audio.examples/E10.complex.FM.pd
new file mode 100644
index 00000000..094d68ed
--- /dev/null
+++ b/desiredata/doc/3.audio.examples/E10.complex.FM.pd
@@ -0,0 +1,156 @@
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+#X obj 18 129 phasor~;
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+#X text 437 472 updated for Pd version 0.37;
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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 14 319 At load time \, calculate a good choice of fundamental
+frequency for showing spectra: the 16th bin in a 4096-point spectrum
+\, so SR*16/4096 or SR/256.;
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+#X obj 220 234 inlet;
+#X text 273 232 toggle to graph repeatedly;
+#X text 262 212 bang to graph once;
+#X obj 16 494 t b f;
+#X obj 19 295 tabwrite~ E10-signal;
+#X obj 208 295 tabwrite~ E10-spectrum;
+#X text 72 536 set carrier multiplier and modulation multipliers after
+fundamental;
+#X msg 16 516 \; cm 8 \; m1 2 \; m2 3;
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+#X text 434 268 -- partial number --;
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+#X text 43 3 SPECTRUM OF COMPLEX PHASE MODULATION;
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+#X text 126 349 Now we introduce a second modulator oscillator. The
+carrier is on the 8th harmonic and the two modulators are at 2 and
+3 times the fundamental. When either index of modulation is zero \,
+changing the other index gives the familiar 2-operator FM result. But
+if index2 is nonzero (try around 10 \, for example) then sliding index1
+upward from 0 introduces sidebands around each of the sidebands.;
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-- 
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