<?xml version="1.0" encoding="UTF-8" standalone="no"?> <!DOCTYPE html PUBLIC "-//W3C//DTD XHTML 1.0 Transitional//EN" "http://www.w3.org/TR/xhtml1/DTD/xhtml1-transitional.dtd"> <html xmlns="http://www.w3.org/1999/xhtml"> <head> <meta http-equiv="Content-Type" content="text/html; charset=UTF-8" /> <title>GEN13</title> <link rel="stylesheet" type="text/css" href="csound.css" /> <meta name="generator" content="DocBook XSL Stylesheets V1.76.1" /> <link rel="home" href="index.html" title="The Canonical Csound Reference Manual" /> <link rel="up" href="ScoregensTop.html" title="Score Statements and GEN Routines" /> <link rel="prev" href="GEN12.html" title="GEN12" /> <link rel="next" href="GEN14.html" title="GEN14" /> </head> <body> <div class="navheader"> <table width="100%" summary="Navigation header"> <tr> <th colspan="3" align="center">GEN13</th> </tr> <tr> <td width="20%" align="left"><a accesskey="p" href="GEN12.html">Prev</a> </td> <th width="60%" align="center">Score Statements and GEN Routines</th> <td width="20%" align="right"> <a accesskey="n" href="GEN14.html">Next</a></td> </tr> </table> <hr /> </div> <div class="refentry" title="GEN13"> <a id="GEN13"></a> <div class="titlepage"></div> <a id="IndexGEN13" class="indexterm"></a> <div class="refnamediv"> <h2> <span class="refentrytitle">GEN13</span> </h2> <p>GEN13 — Stores a polynomial whose coefficients derive from the Chebyshev polynomials of the first kind. </p> </div> <div class="refsect1" title="Description"> <a id="idp77557920"></a> <h2>Description</h2> <p> Uses Chebyshev coefficients to generate stored polynomial functions which, under waveshaping, can be used to split a sinusoid into harmonic partials having a pre-definable spectrum. </p> </div> <div class="refsect1" title="Syntax"> <a id="idp77558920"></a> <h2>Syntax</h2> <pre class="synopsis"><span class="command"><strong>f</strong></span> # time size 13 xint xamp h0 h1 h2 ...</pre> </div> <div class="refsect1" title="Initialization"> <a id="idp77569240"></a> <h2>Initialization</h2> <p> <span class="emphasis"><em>size</em></span> -- number of points in the table. Must be a power of 2 or a power-of-2 plus 1 (see <a class="link" href="f.html" title="f Statement (or Function Table Statement)"><em class="citetitle">f statement</em></a>). The normal value is power-of-2 plus 1. </p> <p> <span class="emphasis"><em>xint</em></span> -- provides the left and right values [<span class="emphasis"><em>-xint, +xint</em></span>] of the x interval over which the polynomial is to be drawn. These subroutines both call <a class="link" href="GEN03.html" title="GEN03"><em class="citetitle">GEN03</em></a> to draw their functions; the p5 value here is therefor expanded to a negative-positive p5, p6 pair before <span class="emphasis"><em>GEN03</em></span> is actually called. The normal value is 1. </p> <p> <span class="emphasis"><em>xamp </em></span> -- amplitude scaling factor of the sinusoid input that is expected to produce the following spectrum. </p> <p> <span class="emphasis"><em>h0, h1, h2,</em></span> etc. -- relative strength of partials 0 (DC), 1 (fundamental), 2 ... that will result when a sinusoid of amplitude </p> <div class="literallayout"> <p><br /> xamp * int(size/2)/xint<br /> </p> </div> <p> is waveshaped using this function table. These values thus describe a frequency spectrum associated with a particular factor <span class="emphasis"><em>xamp</em></span> of the input signal. </p> <p> <span class="emphasis"><em>GEN13</em></span> is the function generator normally employed in standard waveshaping. It stores a polynomial whose coefficients derive from the Chebyshev polynomials of the first kind, so that a driving sinusoid of strength <span class="emphasis"><em>xamp</em></span> will exhibit the specified spectrum at output. Note that the evolution of this spectrum is generally not linear with varying <span class="emphasis"><em>xamp</em></span>. However, it is bandlimited (the only partials to appear will be those specified at generation time); and the partials will tend to occur and to develop in ascending order (the lower partials dominating at low <span class="emphasis"><em>xamp</em></span>, and the spectral richness increasing for higher values of <span class="emphasis"><em>xamp</em></span>). A negative <span class="emphasis"><em>hn</em></span> value implies a 180 degree phase shift of that partial; the requested full-amplitude spectrum will not be affected by this shift, although the evolution of several of its component partials may be. The pattern +,+,-,-,+,+,... for <span class="emphasis"><em>h0,h1,h2..</em></span>. will minimize the normalization problem for low <span class="emphasis"><em>xamp</em></span> values (see above), but does not necessarily provide the smoothest pattern of evolution. </p> </div> <div class="refsect1" title="Examples"> <a id="idp77610224"></a> <h2>Examples</h2> <p> Here is an example of the GEN13 opcode. It uses the file <a class="ulink" href="examples/gen13.csd" target="_top"><em class="citetitle">gen13.csd</em></a>. </p> <div class="example"> <a id="idp77611208"></a> <p class="title"> <strong>Example 1049. Example of the GEN13 opcode.</strong> </p> <div class="example-contents"> <p>See the sections <a class="link" href="UsingRealTime.html" title="Real-Time Audio"><em class="citetitle">Real-time Audio</em></a> and <a class="link" href="CommandFlags.html" title="Csound command line"><em class="citetitle">Command Line Flags</em></a> for more information on using command line flags.</p> <pre class="programlisting"> <span class="csdtag"><CsoundSynthesizer></span> <span class="csdtag"><CsOptions></span> <span class="comment">; Select audio/midi flags here according to platform</span> -odac <span class="comment">;;;realtime audio out</span> <span class="comment">;-iadc ;;;uncomment -iadc if realtime audio input is needed too</span> <span class="comment">; For Non-realtime ouput leave only the line below:</span> <span class="comment">; -o gen13.wav -W ;;; for file output any platform</span> <span class="csdtag"></CsOptions></span> <span class="csdtag"><CsInstruments></span> <span class="ohdr">sr</span> <span class="op">=</span> 44100 <span class="ohdr">ksmps</span> <span class="op">=</span> 32 <span class="ohdr">nchnls</span> <span class="op">=</span> 2 <span class="ohdr">0dbfs</span> <span class="op">=</span> 1 <span class="comment">;example by Russell Pinkston - Univ. of Texas (but slightly modified)</span> gisine <span class="ohdr">ftgen</span> 0, 0, 16384, 10, 1 <span class="comment">;sine wave</span> <span class="oblock">instr</span> 1 ihertz <span class="op">=</span> <span class="opc">cpspch</span>(p4) ipkamp <span class="op">=</span> p5 iwsfn <span class="op">=</span> p6 <span class="comment">;waveshaping function</span> inmfn <span class="op">=</span> p7 <span class="comment">;normalization function</span> agate <span class="opc">linen</span> 1, .01, p3, .1 <span class="comment">;overall amp envelope</span> kctrl <span class="opc">linen</span> .99, 2, p3, 2 <span class="comment">;waveshaping index control</span> aindex <span class="opc">poscil</span> kctrl<span class="op">/</span>2, ihertz, gisine <span class="comment">;sine wave to be distorted</span> asignal <span class="opc">tablei</span> .5<span class="op">+</span>aindex, iwsfn, 1 <span class="comment">;waveshaping</span> knormal <span class="opc">tablei</span> kctrl, inmfn, 1 <span class="comment">;amplitude normalization</span> asig <span class="op">=</span> asignal<span class="op">*</span>knormal<span class="op">*</span>ipkamp<span class="op">*</span>agate <span class="opc">outs</span> asig, asig <span class="oblock">endin</span> <span class="csdtag"></CsInstruments></span> <span class="csdtag"><CsScore></span> <span class="comment">; This proves the statement in Dodge (p. 147) that Chebyshev polynomials</span> <span class="comment">; of order K have "only the kth harmonic." This is only true when the </span> <span class="comment">; waveshaping index is at the maximum - i.e., when the entire transfer</span> <span class="comment">; function is being accessed. RP.</span> <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">; quasi sawtooth transfer function: </span> <span class="comment">; h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16 h17 h18 h19 h20</span> <span class="stamnt">f</span>1 0 513 13 1 1 0 100 -50 -33 25 20 -16.7 -14.2 12.5 11.1 -10 -9.09 8.333 7.69 -7.14 -6.67 6.25 5.88 -5.55 -5.26 5 <span class="stamnt">f</span>2 0 257 4 1 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 0 4 6.00 .7 1 2 <span class="stamnt">i</span>1 4 . 7.00 . <span class="stamnt">i</span>1 8 . 8.00 . <span class="comment">;-------------------------------------------------------------------------------------------------------------------------------------------- </span> <span class="comment">; quasi square wave transfer function: </span> <span class="comment">; h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16 h17 h18 h19</span> <span class="stamnt">f</span>3 0 513 13 1 1 0 100 0 -33 0 20 0 -14.2 0 11.1 0 -9.09 0 7.69 0 -6.67 0 5.88 0 -5.26 <span class="stamnt">f</span>4 0 257 4 3 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 16 4 6.00 .7 3 4 <span class="stamnt">i</span>1 20 . 7.00 . <span class="stamnt">i</span>1 24 . 8.00 . <span class="comment">;-------------------------------------------------------------------------------------------------------------------------------------------- </span> <span class="comment">; quasi triangle wave transfer function: </span> <span class="comment">; h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16 h17 h18 h19</span> <span class="stamnt">f</span>5 0 513 13 1 1 0 100 0 -11.11 0 4 0 -2.04 0 1.23 0 -.826 0 .59 0 -.444 0 .346 0 -.277 <span class="stamnt">f</span>6 0 257 4 5 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 32 4 6.00 .7 5 6 <span class="stamnt">i</span>1 36 . 7.00 . <span class="stamnt">i</span>1 40 . 8.00 . <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">; transfer function1: h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16</span> <span class="stamnt">f</span>7 0 513 13 1 1 0 1 -.8 0 .6 0 0 0 .4 0 0 0 0 .1 -.2 -.3 .5 <span class="stamnt">f</span>8 0 257 4 7 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 48 4 5.00 .7 7 8 <span class="stamnt">i</span>1 52 . 6.00 . <span class="stamnt">i</span>1 56 . 7.00 . <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">;=========================================================================;</span> <span class="comment">; This demonstrates the use of high partials, sometimes without a ;</span> <span class="comment">; fundamental, to get quasi-inharmonic spectra from waveshaping. ;</span> <span class="comment">;=========================================================================;</span> <span class="comment">; transfer function2: h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16</span> <span class="stamnt">f</span>9 0 513 13 1 1 0 0 0 -.1 0 .3 0 -.5 0 .7 0 -.9 0 1 0 -1 0 <span class="stamnt">f</span>10 0 257 4 9 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 64 4 5.00 .7 9 10 <span class="stamnt">i</span>1 68 . 6.00 . <span class="stamnt">i</span>1 72 . 7.00 . <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">; transfer function3: h0 h1 h2 h3 h4 h5 h6 h7 h8 h9 h10 h11 h12 h13 h14 h15 h16 h17 h18 h19 h17 h18 h19 h20</span> <span class="stamnt">f</span>11 0 513 13 1 1 0 0 0 0 0 0 0 -1 0 1 0 0 -.1 0 .1 0 -.2 .3 0 -.7 0 .2 0 -.1 <span class="stamnt">f</span>12 0 257 4 11 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 80 4 5.00 .7 11 12 <span class="stamnt">i</span>1 84 . 5.06 . <span class="stamnt">i</span>1 88 . 6.00 . <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">;=========================================================================;</span> <span class="comment">; split a sinusoid into 3 odd-harmonic partials of relative strength 5:3:1</span> <span class="comment">;=========================================================================;</span> <span class="comment">;--------------------------------------------------------------------------------------------------------------------------------------------</span> <span class="comment">; transfer function4: h0 h1 h2 h3 h4 h5</span> <span class="stamnt">f</span>13 0 513 13 1 1 0 5 0 3 0 1 <span class="stamnt">f</span>14 0 257 4 13 1 <span class="comment">; normalizing function with midpoint bipolar offset</span> <span class="comment">; st dur pch amp wsfn nmfn</span> <span class="stamnt">i</span>1 96 4 5.00 .7 13 14 <span class="stamnt">i</span>1 100 . 5.06 . <span class="stamnt">i</span>1 104 . 6.00 . <span class="stamnt">e</span> <span class="csdtag"></CsScore></span> <span class="csdtag"></CsoundSynthesizer></span> </pre> </div> </div> <p><br class="example-break" /> <span>These are the diagrams of the waveforms of the GEN13 routines, as used in the example:</span> </p> <div class="mediaobject"> <img src="images/gen13_1.png" alt="f1 0 513 13 1 1 0 100 -50 -33 25 20 -16.7 -14.2 12.5 11.1 -10 -9.09 8.333 7.69 -7.14 -6.67 6.25 5.88 -5.55 -5.26 5 - quasi sawtooth transfer function" /> <div class="caption"> <p>f1 0 513 13 1 1 0 100 -50 -33 25 20 -16.7 -14.2 12.5 11.1 -10 -9.09 8.333 7.69 -7.14 -6.67 6.25 5.88 -5.55 -5.26 5 - quasi sawtooth transfer function</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_2.png" alt="f3 0 513 13 1 1 0 100 0 -33 0 20 0 -14.2 0 11.1 0 -9.09 0 7.69 0 -6.67 0 5.88 0 -5.26 - quasi square wave transfer function" /> <div class="caption"> <p>f3 0 513 13 1 1 0 100 0 -33 0 20 0 -14.2 0 11.1 0 -9.09 0 7.69 0 -6.67 0 5.88 0 -5.26 - quasi square wave transfer function</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_3.png" alt="f5 0 513 13 1 1 0 100 0 -11.11 0 4 0 -2.04 0 1.23 0 -.826 0 .59 0 -.444 0 .346 0 -.277 - quasi triangle wave transfer function" /> <div class="caption"> <p>f5 0 513 13 1 1 0 100 0 -11.11 0 4 0 -2.04 0 1.23 0 -.826 0 .59 0 -.444 0 .346 0 -.277 - quasi triangle wave transfer function</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_4.png" alt="f7 0 513 13 1 1 0 1 -.8 0 .6 0 0 0 .4 0 0 0 0 .1 -.2 -.3 .5 - transfer function 1" /> <div class="caption"> <p>f7 0 513 13 1 1 0 1 -.8 0 .6 0 0 0 .4 0 0 0 0 .1 -.2 -.3 .5 - transfer function 1</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_5.png" alt="f9 0 513 13 1 1 0 0 0 -.1 0 .3 0 -.5 0 .7 0 -.9 0 1 0 -1 0 - transfer function 2" /> <div class="caption"> <p>f9 0 513 13 1 1 0 0 0 -.1 0 .3 0 -.5 0 .7 0 -.9 0 1 0 -1 0 - transfer function 2</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_6.png" alt="f11 0 513 13 1 1 0 0 0 0 0 0 0 -1 0 1 0 0 -.1 0 .1 0 -.2 .3 0 -.7 0 .2 0 -.1 - transfer function 3" /> <div class="caption"> <p>f11 0 513 13 1 1 0 0 0 0 0 0 0 -1 0 1 0 0 -.1 0 .1 0 -.2 .3 0 -.7 0 .2 0 -.1 - transfer function 3</p> </div> </div> <p> </p> <div class="mediaobject"> <img src="images/gen13_7.png" alt="f13 0 513 13 1 1 0 5 0 3 0 1 - split a sinusoid into 3 odd-harmonic partials of relative strength 5:3:1" /> <div class="caption"> <p>f13 0 513 13 1 1 0 5 0 3 0 1 - split a sinusoid into 3 odd-harmonic partials of relative strength 5:3:1</p> </div> </div> <p> </p> </div> <div class="refsect1" title="See Also"> <a id="idp77626760"></a> <h2>See Also</h2> <p> <a class="link" href="GEN03.html" title="GEN03"><em class="citetitle">GEN03</em></a>, <a class="link" href="GEN14.html" title="GEN14"><em class="citetitle">GEN14</em></a>, and <a class="link" href="GEN15.html" title="GEN15"><em class="citetitle">GEN15</em></a>. </p> <p> Information about the Chebyshev polynomials on Wikipedia: <a class="ulink" href="http://en.wikipedia.org/wiki/Chebyshev_polynomials" target="_top"><em class="citetitle">http://en.wikipedia.org/wiki/Chebyshev_polynomials</em></a></p> <p> </p> </div> </div> <div class="navfooter"> <hr /> <table width="100%" summary="Navigation footer"> <tr> <td width="40%" align="left"><a accesskey="p" href="GEN12.html">Prev</a> </td> <td width="20%" align="center"> <a accesskey="u" href="ScoregensTop.html">Up</a> </td> <td width="40%" align="right"> <a accesskey="n" href="GEN14.html">Next</a></td> </tr> <tr> <td width="40%" align="left" valign="top">GEN12 </td> <td width="20%" align="center"> <a accesskey="h" href="index.html">Home</a> </td> <td width="40%" align="right" valign="top"> GEN14</td> </tr> </table> </div> </body> </html>