MOS scale: Difference between revisions

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The revision contents are below, presented both in the original Wikispaces Wikitext format, and in HTML exactly as Wikispaces rendered it.<br>
<h4>Original Wikitext content:</h4>
<h4>Original Wikitext content:</h4>
<div style="width:100%; max-height:400pt; overflow:auto; background-color:#f8f9fa; border: 1px solid #eaecf0; padding:0em"><pre style="margin:0px;border:none;background:none;word-wrap:break-word;white-space: pre-wrap ! important" class="old-revision-html">An important class of scales are MOS scales (the acronym **MOS** coming from **"Moment Of Symmetry"**). These are derived by iterating an interval g, called the generator, inside a larger interval, called the period, and reducing to the period when the iterates become larger than the period. Usually the period is an octave or an nth root of 2, but it can in theory be any positive number. The resulting scale is called a MOS, when, as a [[periodic scale]], it has [[http://en.wikipedia.org/wiki/Myhill's_property|Myhill's propery]]: every generic interval aside from the initial unison interval has two specific intervals.  
<div style="width:100%; max-height:400pt; overflow:auto; background-color:#f8f9fa; border: 1px solid #eaecf0; padding:0em"><pre style="margin:0px;border:none;background:none;word-wrap:break-word;white-space: pre-wrap ! important" class="old-revision-html">[[toc|flat]]
----
The term MOS and scale construction method were invented by Erv Wilson in 1975. His original paper can be found here [[http://anaphoria.com/mos.PDF]]. There is also an introduction [[http://anaphoria.com/wilsonintroMOS.html]].In academic music theory, MOS are known as //well-formed scales// and the introduction of the concept is attributed to a 1989 paper by Norman Carey and David Clampitt. A great deal of interesting work has been done on scales in academic circles extending these ideas.


Another characterization of when a generated scale is a MOS is that the number of scale steps is the denominator of a [[http://en.wikipedia.org/wiki/Continued_fraction|convergent or semiconvergent]] of the ratio g/P of the generator and the period. These conditions entail that the generated scale has exactly two sizes of steps when sorted into ascending order of size, and usually that latter condition suffices to define a MOS. However, when the generator is a rational fraction of the period and the number of steps is more than half of the total possible, a generated scale can have only two sizes of steps and the pseudo-Myhill property, meaning that not all non-unison classes have only two specific intervals.
=Definition=
A MOS or Moment Of Symmetry is a scale that consists of:


Note that an octave scale with a period a 1/N fraction of an octave will be a MOS if it is a MOS, identically, within each period.
1. A period "P" (of any size but most commonly the octave or a 1/N fraction of an octave)
2. A generator "g" (of any size, for example 700 cents in 12 equal temperament) which is repeatedly repeatedly added to make a chain of scale steps, starting from the unison or 0 cents scale step, and then reducing to within the period
3. Where there are exactly two two sizes of scale steps (Large and small, often written "L" and "s")
4. Where //each// number of scale steps, or generic interval, within the scale occurs in no more than two different sizes, and in exactly two if the interval is not a multiple of the period
5. The unison or starting point of the scale is then allowed to be transferred to any scale degree--all the modes of a MOS are legal.
 
Condition Four is [[http://en.wikipedia.org/wiki/Myhill's_property|Myhill's propery]] where, as a [[periodic scale]], the scale has every generic interval aside from the initial unison interval and intervals some number of periods from it having exactly two specific intervals. Another characterization of when a generated scale is a MOS is that the number of scale steps is the denominator of a [[http://en.wikipedia.org/wiki/Continued_fraction|convergent or semiconvergent]] of the ratio g/P of the generator and the period.  


The term and scale construction method were invented by Erv Wilson in 1975. His original paper can be found here [[http://anaphoria.com/mos.PDF]]. There is also an introduction [[http://anaphoria.com/wilsonintroMOS.html]].In academic music theory, MOS are known as //well-formed scales// and the introduction of the concept is attributed to a 1989 paper by Norman Carey and David Clampitt. A great deal of interesting work has been done on scales in academic circles extending these ideas.
These conditions entail that the generated scale has exactly two sizes of steps when sorted into ascending order of size, and usually that latter condition suffices to define a MOS. However, when the generator is a rational fraction of the period and the number of steps is more than half of the total possible, a generated scale can have only two sizes of steps and the pseudo-Myhill property, meaning that not all non-unison classes have only two specific intervals.


[[toc|flat]]
Note that an octave scale with a period a 1/N fraction of an octave will be a MOS if it is a MOS, identically, within each period.
----
=The Definition of a Moment of Symmetry=


A moment of Symmetry is a scale that consists of:
1. A generator (of any size, for example a 3/2 or a fifth in 12 equal temperament) which is repeatedly superimposed but reduced within the
2. Interval of Equivalence (of any size for example most commonly the octave)
3. where each scale degree or units will be represented by no more than two sizes and two sizes only (Large and small=L s)
4. and where in turn every number of units within the scale will also occur in no more than two different sizes.
A constant structure (commonly of a higher limit) is a scale where every occurrence of a ratio will always be the same number of steps or units.]
= =  
= =  
=Theory of MOS=  
=Theory of MOS=  
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==[[MOSDiagrams]]== </pre></div>
==[[MOSDiagrams]]== </pre></div>
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<div style="width:100%; max-height:400pt; overflow:auto; background-color:#f8f9fa; border: 1px solid #eaecf0; padding:0em"><pre style="margin:0px;border:none;background:none;word-wrap:break-word;width:200%;white-space: pre-wrap ! important" class="old-revision-html">&lt;html&gt;&lt;head&gt;&lt;title&gt;MOSScales&lt;/title&gt;&lt;/head&gt;&lt;body&gt;An important class of scales are MOS scales (the acronym &lt;strong&gt;MOS&lt;/strong&gt; coming from &lt;strong&gt;&amp;quot;Moment Of Symmetry&amp;quot;&lt;/strong&gt;). These are derived by iterating an interval g, called the generator, inside a larger interval, called the period, and reducing to the period when the iterates become larger than the period. Usually the period is an octave or an nth root of 2, but it can in theory be any positive number. The resulting scale is called a MOS, when, as a &lt;a class="wiki_link" href="/periodic%20scale"&gt;periodic scale&lt;/a&gt;, it has &lt;a class="wiki_link_ext" href="http://en.wikipedia.org/wiki/Myhill's_property" rel="nofollow"&gt;Myhill's propery&lt;/a&gt;: every generic interval aside from the initial unison interval has two specific intervals. &lt;br /&gt;
<div style="width:100%; max-height:400pt; overflow:auto; background-color:#f8f9fa; border: 1px solid #eaecf0; padding:0em"><pre style="margin:0px;border:none;background:none;word-wrap:break-word;width:200%;white-space: pre-wrap ! important" class="old-revision-html">&lt;html&gt;&lt;head&gt;&lt;title&gt;MOSScales&lt;/title&gt;&lt;/head&gt;&lt;body&gt;&lt;!-- ws:start:WikiTextTocRule:24:&amp;lt;img id=&amp;quot;wikitext@@toc@@flat&amp;quot; class=&amp;quot;WikiMedia WikiMediaTocFlat&amp;quot; title=&amp;quot;Table of Contents&amp;quot; src=&amp;quot;/site/embedthumbnail/toc/flat?w=100&amp;amp;h=16&amp;quot;/&amp;gt; --&gt;&lt;!-- ws:end:WikiTextTocRule:24 --&gt;&lt;!-- ws:start:WikiTextTocRule:25: --&gt;&lt;a href="#Definition"&gt;Definition&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:25 --&gt;&lt;!-- ws:start:WikiTextTocRule:26: --&gt; | &lt;a href="#toc1"&gt; &lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:26 --&gt;&lt;!-- ws:start:WikiTextTocRule:27: --&gt; | &lt;a href="#Theory of MOS"&gt;Theory of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:27 --&gt;&lt;!-- ws:start:WikiTextTocRule:28: --&gt; | &lt;a href="#Classification of MOS"&gt;Classification of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:28 --&gt;&lt;!-- ws:start:WikiTextTocRule:29: --&gt;&lt;!-- ws:end:WikiTextTocRule:29 --&gt;&lt;!-- ws:start:WikiTextTocRule:30: --&gt;&lt;!-- ws:end:WikiTextTocRule:30 --&gt;&lt;!-- ws:start:WikiTextTocRule:31: --&gt;&lt;!-- ws:end:WikiTextTocRule:31 --&gt;&lt;!-- ws:start:WikiTextTocRule:32: --&gt;&lt;!-- ws:end:WikiTextTocRule:32 --&gt;&lt;!-- ws:start:WikiTextTocRule:33: --&gt; | &lt;a href="#Catalog of MOS"&gt;Catalog of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:33 --&gt;&lt;!-- ws:start:WikiTextTocRule:34: --&gt; | &lt;a href="#MOS As Applied To Rhythms"&gt;MOS As Applied To Rhythms&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:34 --&gt;&lt;!-- ws:start:WikiTextTocRule:35: --&gt; | &lt;a href="#Algorithms"&gt;Algorithms&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:35 --&gt;&lt;!-- ws:start:WikiTextTocRule:36: --&gt;&lt;!-- ws:end:WikiTextTocRule:36 --&gt;&lt;!-- ws:start:WikiTextTocRule:37: --&gt;
&lt;!-- ws:end:WikiTextTocRule:37 --&gt;&lt;hr /&gt;
The term MOS and scale construction method were invented by Erv Wilson in 1975. His original paper can be found here &lt;a class="wiki_link_ext" href="http://anaphoria.com/mos.PDF" rel="nofollow"&gt;http://anaphoria.com/mos.PDF&lt;/a&gt;. There is also an introduction &lt;a class="wiki_link_ext" href="http://anaphoria.com/wilsonintroMOS.html" rel="nofollow"&gt;http://anaphoria.com/wilsonintroMOS.html&lt;/a&gt;.In academic music theory, MOS are known as &lt;em&gt;well-formed scales&lt;/em&gt; and the introduction of the concept is attributed to a 1989 paper by Norman Carey and David Clampitt. A great deal of interesting work has been done on scales in academic circles extending these ideas.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Another characterization of when a generated scale is a MOS is that the number of scale steps is the denominator of a &lt;a class="wiki_link_ext" href="http://en.wikipedia.org/wiki/Continued_fraction" rel="nofollow"&gt;convergent or semiconvergent&lt;/a&gt; of the ratio g/P of the generator and the period. These conditions entail that the generated scale has exactly two sizes of steps when sorted into ascending order of size, and usually that latter condition suffices to define a MOS. However, when the generator is a rational fraction of the period and the number of steps is more than half of the total possible, a generated scale can have only two sizes of steps and the pseudo-Myhill property, meaning that not all non-unison classes have only two specific intervals.&lt;br /&gt;
&lt;!-- ws:start:WikiTextHeadingRule:0:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc0"&gt;&lt;a name="Definition"&gt;&lt;/a&gt;&lt;!-- ws:end:WikiTextHeadingRule:0 --&gt;Definition&lt;/h1&gt;
A MOS or Moment Of Symmetry is a scale that consists of:&lt;br /&gt;
&lt;br /&gt;
1. A period &amp;quot;P&amp;quot; (of any size but most commonly the octave or a 1/N fraction of an octave)&lt;br /&gt;
2. A generator &amp;quot;g&amp;quot; (of any size, for example 700 cents in 12 equal temperament) which is repeatedly repeatedly added to make a chain of scale steps, starting from the unison or 0 cents scale step, and then reducing to within the period&lt;br /&gt;
3. Where there are exactly two two sizes of scale steps (Large and small, often written &amp;quot;L&amp;quot; and &amp;quot;s&amp;quot;)&lt;br /&gt;
4. Where &lt;em&gt;each&lt;/em&gt; number of scale steps, or generic interval, within the scale occurs in no more than two different sizes, and in exactly two if the interval is not a multiple of the period&lt;br /&gt;
5. The unison or starting point of the scale is then allowed to be transferred to any scale degree--all the modes of a MOS are legal.&lt;br /&gt;
&lt;br /&gt;
Condition Four is &lt;a class="wiki_link_ext" href="http://en.wikipedia.org/wiki/Myhill's_property" rel="nofollow"&gt;Myhill's propery&lt;/a&gt; where, as a &lt;a class="wiki_link" href="/periodic%20scale"&gt;periodic scale&lt;/a&gt;, the scale has every generic interval aside from the initial unison interval and intervals some number of periods from it having exactly two specific intervals. Another characterization of when a generated scale is a MOS is that the number of scale steps is the denominator of a &lt;a class="wiki_link_ext" href="http://en.wikipedia.org/wiki/Continued_fraction" rel="nofollow"&gt;convergent or semiconvergent&lt;/a&gt; of the ratio g/P of the generator and the period. &lt;br /&gt;
&lt;br /&gt;
These conditions entail that the generated scale has exactly two sizes of steps when sorted into ascending order of size, and usually that latter condition suffices to define a MOS. However, when the generator is a rational fraction of the period and the number of steps is more than half of the total possible, a generated scale can have only two sizes of steps and the pseudo-Myhill property, meaning that not all non-unison classes have only two specific intervals.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Note that an octave scale with a period a 1/N fraction of an octave will be a MOS if it is a MOS, identically, within each period.&lt;br /&gt;
Note that an octave scale with a period a 1/N fraction of an octave will be a MOS if it is a MOS, identically, within each period.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The term and scale construction method were invented by Erv Wilson in 1975. His original paper can be found here &lt;a class="wiki_link_ext" href="http://anaphoria.com/mos.PDF" rel="nofollow"&gt;http://anaphoria.com/mos.PDF&lt;/a&gt;. There is also an introduction &lt;a class="wiki_link_ext" href="http://anaphoria.com/wilsonintroMOS.html" rel="nofollow"&gt;http://anaphoria.com/wilsonintroMOS.html&lt;/a&gt;.In academic music theory, MOS are known as &lt;em&gt;well-formed scales&lt;/em&gt; and the introduction of the concept is attributed to a 1989 paper by Norman Carey and David Clampitt. A great deal of interesting work has been done on scales in academic circles extending these ideas.&lt;br /&gt;
&lt;br /&gt;
&lt;!-- ws:start:WikiTextTocRule:24:&amp;lt;img id=&amp;quot;wikitext@@toc@@flat&amp;quot; class=&amp;quot;WikiMedia WikiMediaTocFlat&amp;quot; title=&amp;quot;Table of Contents&amp;quot; src=&amp;quot;/site/embedthumbnail/toc/flat?w=100&amp;amp;h=16&amp;quot;/&amp;gt; --&gt;&lt;!-- ws:end:WikiTextTocRule:24 --&gt;&lt;!-- ws:start:WikiTextTocRule:25: --&gt;&lt;a href="#The Definition of a Moment of Symmetry"&gt;The Definition of a Moment of Symmetry&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:25 --&gt;&lt;!-- ws:start:WikiTextTocRule:26: --&gt; | &lt;a href="#toc1"&gt; &lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:26 --&gt;&lt;!-- ws:start:WikiTextTocRule:27: --&gt; | &lt;a href="#Theory of MOS"&gt;Theory of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:27 --&gt;&lt;!-- ws:start:WikiTextTocRule:28: --&gt; | &lt;a href="#Classification of MOS"&gt;Classification of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:28 --&gt;&lt;!-- ws:start:WikiTextTocRule:29: --&gt;&lt;!-- ws:end:WikiTextTocRule:29 --&gt;&lt;!-- ws:start:WikiTextTocRule:30: --&gt;&lt;!-- ws:end:WikiTextTocRule:30 --&gt;&lt;!-- ws:start:WikiTextTocRule:31: --&gt;&lt;!-- ws:end:WikiTextTocRule:31 --&gt;&lt;!-- ws:start:WikiTextTocRule:32: --&gt;&lt;!-- ws:end:WikiTextTocRule:32 --&gt;&lt;!-- ws:start:WikiTextTocRule:33: --&gt; | &lt;a href="#Catalog of MOS"&gt;Catalog of MOS&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:33 --&gt;&lt;!-- ws:start:WikiTextTocRule:34: --&gt; | &lt;a href="#MOS As Applied To Rhythms"&gt;MOS As Applied To Rhythms&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:34 --&gt;&lt;!-- ws:start:WikiTextTocRule:35: --&gt; | &lt;a href="#Algorithms"&gt;Algorithms&lt;/a&gt;&lt;!-- ws:end:WikiTextTocRule:35 --&gt;&lt;!-- ws:start:WikiTextTocRule:36: --&gt;&lt;!-- ws:end:WikiTextTocRule:36 --&gt;&lt;!-- ws:start:WikiTextTocRule:37: --&gt;
&lt;!-- ws:end:WikiTextTocRule:37 --&gt;&lt;hr /&gt;
&lt;!-- ws:start:WikiTextHeadingRule:0:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc0"&gt;&lt;a name="The Definition of a Moment of Symmetry"&gt;&lt;/a&gt;&lt;!-- ws:end:WikiTextHeadingRule:0 --&gt;The Definition of a Moment of Symmetry&lt;/h1&gt;
&lt;br /&gt;
A moment of Symmetry is a scale that consists of:&lt;br /&gt;
1. A generator (of any size, for example a 3/2 or a fifth in 12 equal temperament) which is repeatedly superimposed but reduced within the&lt;br /&gt;
2. Interval of Equivalence (of any size for example most commonly the octave)&lt;br /&gt;
3. where each scale degree or units will be represented by no more than two sizes and two sizes only (Large and small=L s)&lt;br /&gt;
4. and where in turn every number of units within the scale will also occur in no more than two different sizes.&lt;br /&gt;
A constant structure (commonly of a higher limit) is a scale where every occurrence of a ratio will always be the same number of steps or units.]&lt;br /&gt;
&lt;!-- ws:start:WikiTextHeadingRule:2:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc1"&gt;&lt;!-- ws:end:WikiTextHeadingRule:2 --&gt; &lt;/h1&gt;
&lt;!-- ws:start:WikiTextHeadingRule:2:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc1"&gt;&lt;!-- ws:end:WikiTextHeadingRule:2 --&gt; &lt;/h1&gt;
  &lt;!-- ws:start:WikiTextHeadingRule:4:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc2"&gt;&lt;a name="Theory of MOS"&gt;&lt;/a&gt;&lt;!-- ws:end:WikiTextHeadingRule:4 --&gt;Theory of MOS&lt;/h1&gt;
  &lt;!-- ws:start:WikiTextHeadingRule:4:&amp;lt;h1&amp;gt; --&gt;&lt;h1 id="toc2"&gt;&lt;a name="Theory of MOS"&gt;&lt;/a&gt;&lt;!-- ws:end:WikiTextHeadingRule:4 --&gt;Theory of MOS&lt;/h1&gt;