From 64fdb009695828b788fce074135b20a5e52c5fc4 Mon Sep 17 00:00:00 2001
From: Thomas Grill <xovo@users.sourceforge.net>
Date: Tue, 23 Sep 2003 00:21:28 +0000
Subject: imported version 0.37-0

svn path=/trunk/; revision=1016
---
 pd/doc/5.reference/fft~.pd | 64 ----------------------------------------------
 1 file changed, 64 deletions(-)
 delete mode 100644 pd/doc/5.reference/fft~.pd

(limited to 'pd/doc/5.reference/fft~.pd')

diff --git a/pd/doc/5.reference/fft~.pd b/pd/doc/5.reference/fft~.pd
deleted file mode 100644
index 149a6634..00000000
--- a/pd/doc/5.reference/fft~.pd
+++ /dev/null
@@ -1,64 +0,0 @@
-#N canvas 22 7 886 436 12;
-#X text 85 158 frequency;
-#X floatatom 16 173 0 0 0;
-#X obj 16 120 * 44100;
-#X floatatom 16 94 0 0 0;
-#X text 88 92 frequency;
-#X text 91 111 in bins;
-#X text 85 175 in Hz.;
-#X obj 16 229 osc~;
-#X obj 36 16 fft~;
-#X obj 86 17 ifft~;
-#X text 146 15 - forward and inverse complex FFT;
-#X obj 36 42 rfft~;
-#X obj 86 43 rifft~;
-#X text 146 41 - forward and inverse real FFT;
-#X obj 16 254 rfft~;
-#X obj 16 148 / 64;
-#X obj 574 21 loadbang;
-#X msg 574 47 \; pd dsp 1;
-#X text 636 403 updated for Pd version 0.33;
-#X obj 16 322 rifft~;
-#X obj 102 310 print~ real;
-#X obj 115 285 print~ imaginary;
-#X obj 16 352 /~ 64;
-#X obj 16 407 print~ resynthesized;
-#X msg 30 380 bang;
-#X msg 101 248 bang;
-#X msg 100 199 0.25;
-#X msg 152 199 0;
-#X text 195 200 <-- bash phase;
-#X text 152 249 <-- print analysis;
-#X text 79 380 <-- print resynthesis;
-#X text 76 352 <-- renormalize;
-#X text 347 294 There is no normalization \, so that an FFT followed
-by an IFFT has a gain of N.;
-#X text 346 343 See the FFT examples to see how to use these in practice.
-;
-#X text 346 112 The FFT objects do Fourier analyses and resyntheses
-of incoming real or complex signals. Complex signals are handled as
-pairs of signals (real and imaginary part.) The analysis size is one
-block (you can use the block~ or switch~ obejcts to control block size).
-;
-#X text 347 205 The real FFT outputs N/2+1 real parts and N/2-1 imaginary
-parts. The other outputs are zero. At DC and at the Nyquist there is
-no imaginary part \, but the second through Nth output is as a real
-and imaginary pair \, which can be thought of as the cosine and sin
-component strengths.;
-#X connect 1 0 7 0;
-#X connect 2 0 15 0;
-#X connect 3 0 2 0;
-#X connect 7 0 14 0;
-#X connect 14 0 20 0;
-#X connect 14 0 19 0;
-#X connect 14 1 21 0;
-#X connect 14 1 19 1;
-#X connect 15 0 1 0;
-#X connect 16 0 17 0;
-#X connect 19 0 22 0;
-#X connect 22 0 23 0;
-#X connect 24 0 23 0;
-#X connect 25 0 20 0;
-#X connect 25 0 21 0;
-#X connect 26 0 7 1;
-#X connect 27 0 7 1;
-- 
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