MOS scale: Difference between revisions
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== Examples == | == Examples == | ||
The most widely used MOS scale is the [[5L 2s|diatonic scale]]. It has 7 steps: 5 large ones (major 2nds) and 2 small ones (minor 2nds), and thus is named 5L 2s. The major mode is LLsLLLs. The other modes are rotations of this pattern (e.g. LsLLsLL is the minor mode). | The most widely used MOS scale is the [[5L 2s|diatonic scale]]. It has 7 steps: 5 large ones (major 2nds) and 2 small ones (minor 2nds), and thus is named 5L 2s. The major mode is LLsLLLs. The other modes are rotations of this pattern (e.g. LsLLsLL is the minor mode). | ||
{| class="wikitable" | {| class="wikitable" | ||
|+ | |+ style="font-size: 105%;" | Interval classes in the 5L 2s MOS scale | ||
! rowspan="2" | | |- | ||
! colspan="2" | | ! rowspan="2" | Interval class | ||
! colspan="2" | | ! colspan="2" | Small version | ||
! colspan="2" | Large version | |||
|- | |- | ||
! | ! Quality | ||
! | ! Size | ||
! | ! Quality | ||
! | ! Size | ||
|- | |- | ||
!2nds (1 step) | ! 2nds (1 step) | ||
|minor | | minor | ||
|s | | s | ||
|major | | major | ||
|L | | L | ||
|- | |- | ||
!3rds (2 steps) | ! 3rds (2 steps) | ||
|minor | | minor | ||
|1L + 1s | | {{nowrap|1L + 1s}} | ||
|major | | major | ||
|2L | | 2L | ||
|- | |- | ||
!4ths (3 steps) | ! 4ths (3 steps) | ||
|perfect | | perfect | ||
|2L + 1s | | {{nowrap|2L + 1s}} | ||
|augmented | | augmented | ||
|3L | | 3L | ||
|- | |- | ||
!5ths (4 steps) | ! 5ths (4 steps) | ||
|diminished | | diminished | ||
|2L + 2s | | {{nowrap|2L + 2s}} | ||
|perfect | | perfect | ||
|3L + 1s | | {{nowrap|3L + 1s}} | ||
|- | |- | ||
!6ths (5 steps) | ! 6ths (5 steps) | ||
|minor | | minor | ||
|3L + 2s | | {{nowrap|3L + 2s}} | ||
|major | | major | ||
|4L + 1s | | {{nowrap|4L + 1s}} | ||
|- | |- | ||
!7ths (6 steps) | ! 7ths (6 steps) | ||
|minor | | minor | ||
|4L + 2s | | {{nowrap|4L + 2s}} | ||
|major | | major | ||
|5L + 1s | | {{nowrap|5L + 1s}} | ||
|- | |- | ||
!8ves (7 steps) | ! 8ves (7 steps) | ||
|perfect | | perfect | ||
|5L + 2s | | {{nowrap|5L + 2s}} | ||
| colspan="2" |(only one version) | | colspan="2" | (only one version) | ||
|} | |} | ||
Note that the melodic minor scale (LsLLLLs) has only two step sizes, but it is not MOS since it has three different sizes of fifths: perfect, diminished, and augmented. | Note that the melodic minor scale (LsLLLLs) has only two step sizes, but it is not MOS since it has three different sizes of fifths: perfect, diminished, and augmented. | ||
Other MOS scales include [[2L 3s]], where among its 5 modes are the major pentatonic scale (ssLsL) and the minor pentatonic scale (LssLs), and less commonly [[4L 4s]], also known as the octatonic scale in 12edo, which alternates between large and small steps and comes in two modes (LsLsLsLs and sLsLsLsL). | Other MOS scales include [[2L 3s]], where among its 5 modes are the major pentatonic scale (ssLsL) and the minor pentatonic scale (LssLs), and less commonly [[4L 4s]], also known as the octatonic scale in 12edo, which alternates between large and small steps and comes in two modes (LsLsLsLs and sLsLsLsL). | ||
See the [[catalog of MOS]] for other MOS scales. | See the [[catalog of MOS]] for other MOS scales. | ||
== Periods and generators == | == Periods and generators == | ||
Every MOS scale can be ''generated'' by stacking a certain interval called the [[generator]] and octave-reducing (or more generally, [[period]]-reducing). For example, the diatonic scale is generated by stacking 6 fifths (or equivalently, 6 fourths) and octave-reducing to get a 7 note scale. Another example, 2L 3s is generated by stacking 4 fifths to get 5 notes. However, stacking 5 fifths to get a hexatonic scale such as C D E F G A C does not produces a MOS, because there are more than 2 sizes of each interval class. | Every MOS scale can be ''generated'' by stacking a certain interval called the [[generator]] and octave-reducing (or more generally, [[period]]-reducing). For example, the diatonic scale is generated by stacking 6 fifths (or equivalently, 6 fourths) and octave-reducing to get a 7 note scale. Another example, 2L 3s is generated by stacking 4 fifths to get 5 notes. However, stacking 5 fifths to get a hexatonic scale such as {{nowrap| C D E F G A C }} does not produces a MOS, because there are more than 2 sizes of each interval class. | ||
The amount of stacking that produces a MOS scale depends only on the size of the generator relative to the size to the period. For a just fifth and a just octave, the valid scale sizes are 2, 3, 5, 7, 12, 17, 29, 41, 53 | The amount of stacking that produces a MOS scale depends only on the size of the generator relative to the size to the period. For a just fifth and a just octave, the valid scale sizes are 2, 3, 5, 7, 12, 17, 29, 41, 53, …. However for a quarter-comma meantone fifth, the valid sizes are 2, 3, 5, 7, 12, 19, 31, 50, …. | ||
== Step ratio spectrum == | == Step ratio spectrum == | ||
The [[step ratio]] is the ratio of the larger step size to the smaller step size. MOSes with smaller step ratios sound smooth and soft. MOSes with larger step ratios sound jagged and hard. Different step ratios produce different corresponding potential temperament interpretations. The [[TAMNAMS#Step ratio spectrum|TAMNAMS]] system has names for specific ratios and also ranges of ratios. | The [[step ratio]] is the ratio of the larger step size to the smaller step size. MOSes with smaller step ratios sound smooth and soft. MOSes with larger step ratios sound jagged and hard. Different step ratios produce different corresponding potential temperament interpretations. The [[TAMNAMS #Step ratio spectrum|TAMNAMS]] system has names for specific ratios and also ranges of ratios. | ||
When the step ratio is a rational number, the MOS is tuned to an edo. A counter-example is 5L 2s tuned to quarter-comma meantone, which has a step ratio of about 1.649. | When the step ratio is a rational number, the MOS is tuned to an edo. A counter-example is 5L 2s tuned to quarter-comma meantone, which has a step ratio of about 1.649. | ||
{| class="wikitable" | {| class="wikitable" | ||
|+5L 2s step ratios in various edos | |+ style="font-size: 105%;" | 5L 2s step ratios in various edos | ||
|- | |- | ||
! | ! Example edo | ||
! Step ratio | |||
! TAMNAMS name | |||
! Likely temperament<br />interpretations | |||
|- | |- | ||
! | ! 12 | ||
| | | 2:1 | ||
| | | basic | ||
|[[Meantone]] | | [[Meantone]] or [[Schismatic]] | ||
|- | |- | ||
!22 | ! 19 | ||
|4:1 | | 3:2 | ||
|superhard | | soft | ||
|[[Archy]] or [[Superpyth]] | | [[Meantone]] | ||
|- | |||
! 22 | |||
| 4:1 | |||
| superhard | |||
| [[Archy]] or [[Superpyth]] | |||
|} | |} | ||
== Naming == | == Naming == | ||
Every MOS can be uniquely specified by giving its [[signature]], i.e. the number of large and small steps, which is typically notated e.g. "5L 2s,". Every possible signature corresponds to a valid MOS scale. Sometimes, if one simply wants to talk about step sizes without specifying which is large and small, the notation "5a 2b" is used (which could refer to either diatonic or [[2L 5s|anti-diatonic]] = 2L 5s). | Every MOS can be uniquely specified by giving its [[signature]], i.e. the number of large and small steps, which is typically notated e.g. "5L 2s,". Every possible signature corresponds to a valid MOS scale. Sometimes, if one simply wants to talk about step sizes without specifying which is large and small, the notation "5a 2b" is used (which could refer to either diatonic or {{nowrap| [[2L 5s|anti-diatonic]] {{=}} 2L 5s }}). | ||
By default, the [[equave]] of a MOS is assumed to be [[2/1]]. To specify a non-octave equave, "{{angbr|equave}}" is placed after the signature, e.g. {{mos scalesig|4L 5s<3/1>|link=1}}. Using angle brackets (<code>&#x27E8;</code> and <code>&#x27E9;</code>) is recommended; using greater-than and less-than signs ("<equave>") can also be done, but this can conflict with HTML and other uses of these symbols. | By default, the [[equave]] of a MOS is assumed to be [[2/1]]. To specify a non-octave equave, "{{angbr|equave}}" is placed after the signature, e.g. {{mos scalesig|4L 5s<3/1>|link=1}}. Using angle brackets (<code>&#x27E8;</code> and <code>&#x27E9;</code>) is recommended; using greater-than and less-than signs ("<equave>") can also be done, but this can conflict with HTML and other uses of these symbols. | ||
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The term ''MOS'', and the method of scale construction it entails, were invented by [[Erv Wilson]] in 1975. His original paper is archived on Anaphoria.com here: [https://anaphoria.com/mos.pdf ''Moments of Symmetry'']. There is also an introduction by [[Kraig Grady]] here: [https://anaphoria.com/wilsonintroMOS.html ''Introduction to Erv Wilson's Moments of Symmetry'']. | The term ''MOS'', and the method of scale construction it entails, were invented by [[Erv Wilson]] in 1975. His original paper is archived on Anaphoria.com here: [https://anaphoria.com/mos.pdf ''Moments of Symmetry'']. There is also an introduction by [[Kraig Grady]] here: [https://anaphoria.com/wilsonintroMOS.html ''Introduction to Erv Wilson's Moments of Symmetry'']. | ||
Sometimes, scales are defined with respect to a period and an additional [[equivalence interval]], the interval at which pitch classes repeat. MOSes in which the equivalence interval is a multiple of the period, and in which there is more than one period per equivalence interval, are sometimes called '''Multi-MOSes'''. MOSes in which the equivalence interval is equal to the period are sometimes called '''Strict MOSes'''. MOSes in which the equivalence interval and period are simply disjunct, with no rational relationship between them, are simply MOS and have no additional distinguishing label. | Sometimes, scales are defined with respect to a period and an additional [[equivalence interval]], the interval at which pitch classes repeat. MOSes in which the equivalence interval is a multiple of the period, and in which there is more than one period per equivalence interval, are sometimes called '''Multi-MOSes'''. For example, a MOS with a half-octave period is called a '''2mos''', with a 1/3-octave period a '''3mos''', and so on. MOSes in which the equivalence interval is equal to the period are sometimes called '''Strict MOSes'''. MOSes in which the equivalence interval and period are simply disjunct, with no rational relationship between them, are simply MOS and have no additional distinguishing label. | ||
With a few notable exceptions, Wilson generally focused his attention on MOS with period equal to the equivalence interval. Hence, some people prefer to use the term [[Distributional evenness|distributionally even scale]], with acronym DE, for the more general class of scales which are MOS with respect to other intervals. MOS/DE scales are also sometimes known as ''well-formed scales'', the term used in the 1989 paper by Norman Carey and David Clampitt<ref>Norman Carey and David Clampitt. "Aspects of Well-Formed Scales", ''Music Theory Spectrum'', Vol. 11, No. 2 (Autumn, 1989), pp. 187-206.</ref>. A great deal of work has been done in academic circles extending these ideas. The idea of MOS also includes secondary or bi-level MOS scales which are actually the inspiration of Wilson's concept. They are in a sense the MOS of MOS patterns. This is used to explain the [[ | With a few notable exceptions, Wilson generally focused his attention on MOS with period equal to the equivalence interval. Hence, some people prefer to use the term [[Distributional evenness|distributionally even scale]], with acronym DE, for the more general class of scales which are MOS with respect to other intervals. MOS/DE scales are also sometimes known as ''well-formed scales'', the term used in the 1989 paper by Norman Carey and David Clampitt<ref>Norman Carey and David Clampitt. "Aspects of Well-Formed Scales", ''Music Theory Spectrum'', Vol. 11, No. 2 (Autumn, 1989), pp. 187-206.</ref>. A great deal of work has been done in academic circles extending these ideas. The idea of MOS also includes secondary or bi-level MOS scales which are actually the inspiration of Wilson's concept. They are in a sense the MOS of MOS patterns. This is used to explain the [[pentatonic]]s used in traditional [[Japanese music]] (e.g. {{nowrap| A B C E F A }}), where the 5-tone cycles are derived from a 7-tone MOS, which are not found in the concept of DE. | ||
== Equivalent definitions and generalizations == | == Equivalent definitions and generalizations == | ||
A scale is a MOS if and only if it satisfies one of the following equivalent criteria: | A scale is a MOS if and only if it satisfies one of the following equivalent criteria: | ||
# [[Maximum variety]] 2: Ascending by a certain number of steps is equivalent to ascending by one of at most two intervals, and the maximum of two is achieved (i. e. it is not true that ascending by a certain number of steps is always equivalent to ascending by one interval.) | # [[Maximum variety]] 2: Ascending by a certain number of steps is equivalent to ascending by one of at most two intervals, and the maximum of two is achieved (i. e. it is not true that ascending by a certain number of steps is always equivalent to ascending by one interval.) | ||
# [[Binary]] and has a [[generator]]: The scale step comes in exactly two sizes, and the scale is formable from stacking some interval called a generator and octave-reducing. | # [[Binary]] and has a [[generator]]: The scale step comes in exactly two sizes, and the scale is formable from stacking some interval called a generator and octave-reducing. | ||
# Mode of a Christoffel word: The scale can be formed by creating a 2D lattice where the period is on the lattice, then taking pitches by travelling vertically and horizontally from the origin, maintaining as close to the line from the origin to the octave as possible without going above it. | # Mode of a Christoffel word: The scale can be formed by creating a 2D lattice where the period is on the lattice, then taking pitches by travelling vertically and horizontally from the origin, maintaining as close to the line from the origin to the octave as possible without going above it. | ||
Each definition generalizes to scales with three or more step sizes, but these generalizations are not equivalent. The concepts of [[ | Each definition generalizes to scales with three or more step sizes, but these generalizations are not equivalent. The concepts of [[balanced word|balance]] and [[distributional evenness]] provide still different generalizations, although defining MOS through these terms is less helpful. For more information, see [[Mathematics of MOS]]. | ||
== Properties == | == Properties == | ||
=== Basic properties === | === Basic properties === | ||
* For every MOS scale with an [[octave]] period (which is usually the [[octave]]), if ''x''-[[edo]] is the [[collapsed]] tuning (where the small step vanishes) and ''y''-[[edo]] is the [[equalized]] tuning (where the large (''L'') step and small (''s'') step are the same size), then by definition it is an {{nowrap| ''x''L (''y'' − ''x'')s }} MOS scale, and the [[basic]] tuning where {{nowrap| ''L'' {{=}} 2''s'' }} is thus {{nowrap|(''x'' + ''y'')}}-[[edo]]. This is also true if the period is 1\''p'', that is, 1 step of ''p''-[[edo]], which implies that ''x'' and ''y'' are divisible by ''p'', though note that in that case (if {{nowrap| ''p'' > 1 }}) you are considering a "multiperiod" MOS scale. | |||
* More generally, whenever ''px''-[[edo]] and ''py''-[[edo]] are used to define two [[val]]s (usually but not necessarily through taking the [[Patent val|patent vals]]) while simultaneously also being used to define the {{nowrap|''px''L (''py'' − ''px'')s}} MOS scale (where ''p'' is the number of periods per octave), then the ''px'' & ''py'' temperament corresponds to that MOS scale, and adding ''x'' and/or ''y'' corresponds to tuning closer to ''x''-[[edo]] and/or ''y''-[[edo]] respectively. (Optionally, see the below more precise statement for the mathematically-inclined.) | |||
* For the mathematically-inclined, we can say that whenever we consider a MOS with ''X''/''p'' notes per period in the [[collapsed]] tuning and ''Y''/''p'' notes per period in the [[equalized]] tuning and ''p'' periods per [[Octave stretching|tempered octave]] (or more generally tempered [[equave]]), and whenever we want to associate that MOS with the {{nowrap| ''X'' & ''Y'' }} rank 2 temperament'''*''', we can say that any {{w|natural number|natural}}-coefficient {{w|linear combination}} of vals {{val| ''X'' … }} and {{val| ''Y'' … }} (where {{nowrap| ''X'' < ''Y'' }}) corresponds uniquely to a tuning of the {{nowrap| ''X'' & ''Y'' }} rank 2 temperament between ''X''-[[ET]] and ''Y''-[[ET]] (inclusive) iff {{nowrap| gcd(''a'', ''b'') {{=}} 1 }}, because if {{nowrap| ''k'' {{=}} gcd(''a'', ''b'') > 1 }} then the val {{nowrap| ''a''{{val| ''X'' … }} + ''b''{{val| ''Y'' … }} }} has a common factor ''k'' in all of its terms, meaning it is guaranteed to be [[contorted]]. The tuning corresponding to the {{w|Rational number|rational}} ''a''/''b'' is technically only unique up to (discarding of) [[octave stretching]] (or more generally [[equave]]-tempering). | |||
: The period of this temperament is {{nowrap|1\gcd(''X'', ''Y'')}}, and the rational ''a''/''b'' is very closely related to the [[step ratio]] of the corresponding MOS scale, because {{nowrap| 1{{val| ''X'' … }} + 0{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 1|''s'' {{=}} 0}} tuning while {{nowrap| 0{{val| ''X'' … }} + 1{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 1|''s'' {{=}} 1}} tuning and {{nowrap| 1{{val| ''X'' … ;}} + 1{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 2|''s'' {{=}} 1}} tuning, so that {{nowrap|''L'' {{=}} ''a'' + ''b''}} and {{nowrap|''s'' {{=}} ''b''}} and therefore: | |||
: | : {{nowrap|1/([[step ratio]]) {{=}} ''s''/''L''}} {{nowrap|{{=}} ''b''/(''a'' + ''b'')}} implying [[step ratio]] {{nowrap| ''r'' {{=}} (''a'' + ''b'')/''b'' ≥ 1 }} for {{w|Natural number|natural}} ''a'' and ''b'', where if {{nowrap| ''b'' {{=}} 0 }} then the step ratio is infinite, corresponding to the [[collapsed]] tuning.<ref group="note">It is ''important to note'' that the correspondence to the {{nowrap| ''X'' & ''Y'' }} rank-2 temperament only works in all cases if we allow the temperament to be [[contorted]] on its [[subgroup]]; alternatively, it works if we exclude cases where {{nowrap| ''X'' & ''Y'' }} describe a contorted temperament on the subgroup given. An example is the {{nowrap| 5 & 19 }} temperament is contorted in the [[5-limit]] (having a generator of a semifourth, corresponding to [[5L 14s]]), so we either need to consider the temperament itself to be contorted (generated by something lacking an interpretation in the subgroup given, two of which yielding a meantone-tempered [[~]][[4/3]]) or we exclude it because of its contortion.</ref> | ||
* Every MOS scale has two ''child MOS'' scales. The two children of the MOS scale ''a''L ''b''s are {{nowrap| (''a'' + ''b'')L ''a''s }} (generated by generators of soft-of-basic ''a''L ''b''s) and {{nowrap| ''a''L (''a'' + ''b'')s }} (generated by generators of hard-of-basic ''a''L'' b''s). | |||
* Every MOS scale (with a specified [[equave]] ''Ɛ''), excluding {{nowrap|''a''L ''a''s{{angbr|''Ɛ''}} }}, has a ''parent MOS''. If {{nowrap| ''a'' > ''b'' }}, the parent of ''a''L ''b''s is {{nowrap| ''b''L (''a'' − ''b'')s }}; if {{nowrap| ''a'' < ''b'' }}, the parent of ''a''L ''b''s is {{nowrap| ''a''L (''b'' − ''a'')s }}. | |||
* Every MOS scale has two ''child MOS'' scales. The two children of the MOS scale ''a''L ''b''s are {{nowrap|(''a'' + ''b'')L ''a''s}} (generated by generators of soft-of-basic ''a''L ''b''s) and {{nowrap|''a''L (''a'' + ''b'')s}} (generated by generators of hard-of-basic ''a''L'' b''s). | |||
* Every MOS scale (with a specified [[equave]] '' | |||
=== Advanced discussion === | === Advanced discussion === | ||
See: | See: | ||
* [[Mathematics of MOS]], a more formal definition and a discussion of the mathematical properties. | * [[Mathematics of MOS]], a more formal definition and a discussion of the mathematical properties. | ||
** [[Recursive structure of MOS scales]], a description of how MOS scales are recursive and how one scale can be converted into a related scale. | ** [[Recursive structure of MOS scales]], a description of how MOS scales are recursive and how one scale can be converted into a related scale. | ||
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* [[MOS diagrams]], visualizations of the MOS process. | * [[MOS diagrams]], visualizations of the MOS process. | ||
* [http://x31eq.com/temper/method.html How to Find Linear Temperaments], by [[Graham Breed]] | * [http://x31eq.com/temper/method.html How to Find Linear Temperaments], by [[Graham Breed]] | ||
== Individual pages for MOS scales == | |||
=== L ≤ 12, s ≤ 12 === | |||
{| class="wikitable center-all" | |||
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|L ≤ 12|s ≤ 12}}) | |||
|- | |||
| [[1L 1s]] | |||
| [[1L 2s]] | |||
| [[1L 3s]] | |||
| [[1L 4s]] | |||
| [[1L 5s]] | |||
| [[1L 6s]] | |||
| [[1L 7s]] | |||
| [[1L 8s]] | |||
| [[1L 9s]] | |||
| [[1L 10s]] | |||
| [[1L 11s]] | |||
| [[1L 12s]] | |||
|- | |||
| [[2L 1s]] | |||
| [[2L 2s]] | |||
| [[2L 3s]] | |||
| [[2L 4s]] | |||
| [[2L 5s]] | |||
| [[2L 6s]] | |||
| [[2L 7s]] | |||
| [[2L 8s]] | |||
| [[2L 9s]] | |||
| [[2L 10s]] | |||
| [[2L 11s]] | |||
| [[2L 12s]] | |||
|- | |||
| [[3L 1s]] | |||
| [[3L 2s]] | |||
| [[3L 3s]] | |||
| [[3L 4s]] | |||
| [[3L 5s]] | |||
| [[3L 6s]] | |||
| [[3L 7s]] | |||
| [[3L 8s]] | |||
| [[3L 9s]] | |||
| [[3L 10s]] | |||
| [[3L 11s]] | |||
| [[3L 12s]] | |||
|- | |||
| [[4L 1s]] | |||
| [[4L 2s]] | |||
| [[4L 3s]] | |||
| [[4L 4s]] | |||
| [[4L 5s]] | |||
| [[4L 6s]] | |||
| [[4L 7s]] | |||
| [[4L 8s]] | |||
| [[4L 9s]] | |||
| [[4L 10s]] | |||
| [[4L 11s]] | |||
| [[4L 12s]] | |||
|- | |||
| [[5L 1s]] | |||
| [[5L 2s]] | |||
| [[5L 3s]] | |||
| [[5L 4s]] | |||
| [[5L 5s]] | |||
| [[5L 6s]] | |||
| [[5L 7s]] | |||
| [[5L 8s]] | |||
| [[5L 9s]] | |||
| [[5L 10s]] | |||
| [[5L 11s]] | |||
| [[5L 12s]] | |||
|- | |||
| [[6L 1s]] | |||
| [[6L 2s]] | |||
| [[6L 3s]] | |||
| [[6L 4s]] | |||
| [[6L 5s]] | |||
| [[6L 6s]] | |||
| [[6L 7s]] | |||
| [[6L 8s]] | |||
| [[6L 9s]] | |||
| [[6L 10s]] | |||
| [[6L 11s]] | |||
| [[6L 12s]] | |||
|- | |||
| [[7L 1s]] | |||
| [[7L 2s]] | |||
| [[7L 3s]] | |||
| [[7L 4s]] | |||
| [[7L 5s]] | |||
| [[7L 6s]] | |||
| [[7L 7s]] | |||
| [[7L 8s]] | |||
| [[7L 9s]] | |||
| [[7L 10s]] | |||
| [[7L 11s]] | |||
| [[7L 12s]] | |||
|- | |||
| [[8L 1s]] | |||
| [[8L 2s]] | |||
| [[8L 3s]] | |||
| [[8L 4s]] | |||
| [[8L 5s]] | |||
| [[8L 6s]] | |||
| [[8L 7s]] | |||
| [[8L 8s]] | |||
| [[8L 9s]] | |||
| [[8L 10s]] | |||
| [[8L 11s]] | |||
| [[8L 12s]] | |||
|- | |||
| [[9L 1s]] | |||
| [[9L 2s]] | |||
| [[9L 3s]] | |||
| [[9L 4s]] | |||
| [[9L 5s]] | |||
| [[9L 6s]] | |||
| [[9L 7s]] | |||
| [[9L 8s]] | |||
| [[9L 9s]] | |||
| [[9L 10s]] | |||
| [[9L 11s]] | |||
| [[9L 12s]] | |||
|- | |||
| [[10L 1s]] | |||
| [[10L 2s]] | |||
| [[10L 3s]] | |||
| [[10L 4s]] | |||
| [[10L 5s]] | |||
| [[10L 6s]] | |||
| [[10L 7s]] | |||
| [[10L 8s]] | |||
| [[10L 9s]] | |||
| [[10L 10s]] | |||
| [[10L 11s]] | |||
| [[10L 12s]] | |||
|- | |||
| [[11L 1s]] | |||
| [[11L 2s]] | |||
| [[11L 3s]] | |||
| [[11L 4s]] | |||
| [[11L 5s]] | |||
| [[11L 6s]] | |||
| [[11L 7s]] | |||
| [[11L 8s]] | |||
| [[11L 9s]] | |||
| [[11L 10s]] | |||
| [[11L 11s]] | |||
| [[11L 12s]] | |||
|- | |||
| [[12L 1s]] | |||
| [[12L 2s]] | |||
| [[12L 3s]] | |||
| [[12L 4s]] | |||
| [[12L 5s]] | |||
| [[12L 6s]] | |||
| [[12L 7s]] | |||
| [[12L 8s]] | |||
| [[12L 9s]] | |||
| [[12L 10s]] | |||
| [[12L 11s]] | |||
| [[12L 12s]] | |||
|} | |||
=== L ≤ 12, 13 ≤ s ≤ 24 === | |||
{| class="wikitable mw-collapsible mw-collapsed center-all" | |||
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|L ≤ 12|13 ≤ s ≤ 24}}) | |||
|- | |||
| [[1L 13s]] | |||
| [[1L 14s]] | |||
| [[1L 15s]] | |||
| [[1L 16s]] | |||
| [[1L 17s]] | |||
| [[1L 18s]] | |||
| [[1L 19s]] | |||
| [[1L 20s]] | |||
| [[1L 21s]] | |||
| [[1L 22s]] | |||
| [[1L 23s]] | |||
| [[1L 24s]] | |||
|- | |||
| [[2L 13s]] | |||
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| [[2L 17s]] | |||
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| [[2L 22s]] | |||
| [[2L 23s]] | |||
| [[2L 24s]] | |||
|- | |||
| [[3L 13s]] | |||
| [[3L 14s]] | |||
| [[3L 15s]] | |||
| [[3L 16s]] | |||
| [[3L 17s]] | |||
| [[3L 18s]] | |||
| [[3L 19s]] | |||
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| [[3L 22s]] | |||
| [[3L 23s]] | |||
| [[3L 24s]] | |||
|- | |||
| [[4L 13s]] | |||
| [[4L 14s]] | |||
| [[4L 15s]] | |||
| [[4L 16s]] | |||
| [[4L 17s]] | |||
| [[4L 18s]] | |||
| [[4L 19s]] | |||
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| [[4L 21s]] | |||
| [[4L 22s]] | |||
| [[4L 23s]] | |||
| [[4L 24s]] | |||
|- | |||
| [[5L 13s]] | |||
| [[5L 14s]] | |||
| [[5L 15s]] | |||
| [[5L 16s]] | |||
| [[5L 17s]] | |||
| [[5L 18s]] | |||
| [[5L 19s]] | |||
| [[5L 20s]] | |||
| [[5L 21s]] | |||
| [[5L 22s]] | |||
| [[5L 23s]] | |||
| [[5L 24s]] | |||
|- | |||
| [[6L 13s]] | |||
| [[6L 14s]] | |||
| [[6L 15s]] | |||
| [[6L 16s]] | |||
| [[6L 17s]] | |||
| [[6L 18s]] | |||
| [[6L 19s]] | |||
| [[6L 20s]] | |||
| [[6L 21s]] | |||
| [[6L 22s]] | |||
| [[6L 23s]] | |||
| [[6L 24s]] | |||
|- | |||
| [[7L 13s]] | |||
| [[7L 14s]] | |||
| [[7L 15s]] | |||
| [[7L 16s]] | |||
| [[7L 17s]] | |||
| [[7L 18s]] | |||
| [[7L 19s]] | |||
| [[7L 20s]] | |||
| [[7L 21s]] | |||
| [[7L 22s]] | |||
| [[7L 23s]] | |||
| [[7L 24s]] | |||
|- | |||
| [[8L 13s]] | |||
| [[8L 14s]] | |||
| [[8L 15s]] | |||
| [[8L 16s]] | |||
| [[8L 17s]] | |||
| [[8L 18s]] | |||
| [[8L 19s]] | |||
| [[8L 20s]] | |||
| [[8L 21s]] | |||
| [[8L 22s]] | |||
| [[8L 23s]] | |||
| [[8L 24s]] | |||
|- | |||
| [[9L 13s]] | |||
| [[9L 14s]] | |||
| [[9L 15s]] | |||
| [[9L 16s]] | |||
| [[9L 17s]] | |||
| [[9L 18s]] | |||
| [[9L 19s]] | |||
| [[9L 20s]] | |||
| [[9L 21s]] | |||
| [[9L 22s]] | |||
| [[9L 23s]] | |||
| [[9L 24s]] | |||
|- | |||
| [[10L 13s]] | |||
| [[10L 14s]] | |||
| [[10L 15s]] | |||
| [[10L 16s]] | |||
| [[10L 17s]] | |||
| [[10L 18s]] | |||
| [[10L 19s]] | |||
| [[10L 20s]] | |||
| [[10L 21s]] | |||
| [[10L 22s]] | |||
| [[10L 23s]] | |||
| [[10L 24s]] | |||
|- | |||
| [[11L 13s]] | |||
| [[11L 14s]] | |||
| [[11L 15s]] | |||
| [[11L 16s]] | |||
| [[11L 17s]] | |||
| [[11L 18s]] | |||
| [[11L 19s]] | |||
| [[11L 20s]] | |||
| [[11L 21s]] | |||
| [[11L 22s]] | |||
| [[11L 23s]] | |||
| [[11L 24s]] | |||
|- | |||
| [[12L 13s]] | |||
| [[12L 14s]] | |||
| [[12L 15s]] | |||
| [[12L 16s]] | |||
| [[12L 17s]] | |||
| [[12L 18s]] | |||
| [[12L 19s]] | |||
| [[12L 20s]] | |||
| [[12L 21s]] | |||
| [[12L 22s]] | |||
| [[12L 23s]] | |||
| [[12L 24s]] | |||
|} | |||
=== 13 ≤ L ≤ 24, s ≤ 12 === | |||
{| class="wikitable mw-collapsible mw-collapsed center-all" | |||
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|13 ≤ L ≤ 24|s ≤ 12}}) | |||
|- | |||
| [[13L 1s]] | |||
| [[13L 2s]] | |||
| [[13L 3s]] | |||
| [[13L 4s]] | |||
| [[13L 5s]] | |||
| [[13L 6s]] | |||
| [[13L 7s]] | |||
| [[13L 8s]] | |||
| [[13L 9s]] | |||
| [[13L 10s]] | |||
| [[13L 11s]] | |||
| [[13L 12s]] | |||
|- | |||
| [[14L 1s]] | |||
| [[14L 2s]] | |||
| [[14L 3s]] | |||
| [[14L 4s]] | |||
| [[14L 5s]] | |||
| [[14L 6s]] | |||
| [[14L 7s]] | |||
| [[14L 8s]] | |||
| [[14L 9s]] | |||
| [[14L 10s]] | |||
| [[14L 11s]] | |||
| [[14L 12s]] | |||
|- | |||
| [[15L 1s]] | |||
| [[15L 2s]] | |||
| [[15L 3s]] | |||
| [[15L 4s]] | |||
| [[15L 5s]] | |||
| [[15L 6s]] | |||
| [[15L 7s]] | |||
| [[15L 8s]] | |||
| [[15L 9s]] | |||
| [[15L 10s]] | |||
| [[15L 11s]] | |||
| [[15L 12s]] | |||
|- | |||
| [[16L 1s]] | |||
| [[16L 2s]] | |||
| [[16L 3s]] | |||
| [[16L 4s]] | |||
| [[16L 5s]] | |||
| [[16L 6s]] | |||
| [[16L 7s]] | |||
| [[16L 8s]] | |||
| [[16L 9s]] | |||
| [[16L 10s]] | |||
| [[16L 11s]] | |||
| [[16L 12s]] | |||
|- | |||
| [[17L 1s]] | |||
| [[17L 2s]] | |||
| [[17L 3s]] | |||
| [[17L 4s]] | |||
| [[17L 5s]] | |||
| [[17L 6s]] | |||
| [[17L 7s]] | |||
| [[17L 8s]] | |||
| [[17L 9s]] | |||
| [[17L 10s]] | |||
| [[17L 11s]] | |||
| [[17L 12s]] | |||
|- | |||
| [[18L 1s]] | |||
| [[18L 2s]] | |||
| [[18L 3s]] | |||
| [[18L 4s]] | |||
| [[18L 5s]] | |||
| [[18L 6s]] | |||
| [[18L 7s]] | |||
| [[18L 8s]] | |||
| [[18L 9s]] | |||
| [[18L 10s]] | |||
| [[18L 11s]] | |||
| [[18L 12s]] | |||
|- | |||
| [[19L 1s]] | |||
| [[19L 2s]] | |||
| [[19L 3s]] | |||
| [[19L 4s]] | |||
| [[19L 5s]] | |||
| [[19L 6s]] | |||
| [[19L 7s]] | |||
| [[19L 8s]] | |||
| [[19L 9s]] | |||
| [[19L 10s]] | |||
| [[19L 11s]] | |||
| [[19L 12s]] | |||
|- | |||
| [[20L 1s]] | |||
| [[20L 2s]] | |||
| [[20L 3s]] | |||
| [[20L 4s]] | |||
| [[20L 5s]] | |||
| [[20L 6s]] | |||
| [[20L 7s]] | |||
| [[20L 8s]] | |||
| [[20L 9s]] | |||
| [[20L 10s]] | |||
| [[20L 11s]] | |||
| [[20L 12s]] | |||
|- | |||
| [[21L 1s]] | |||
| [[21L 2s]] | |||
| [[21L 3s]] | |||
| [[21L 4s]] | |||
| [[21L 5s]] | |||
| [[21L 6s]] | |||
| [[21L 7s]] | |||
| [[21L 8s]] | |||
| [[21L 9s]] | |||
| [[21L 10s]] | |||
| [[21L 11s]] | |||
| [[21L 12s]] | |||
|- | |||
| [[22L 1s]] | |||
| [[22L 2s]] | |||
| [[22L 3s]] | |||
| [[22L 4s]] | |||
| [[22L 5s]] | |||
| [[22L 6s]] | |||
| [[22L 7s]] | |||
| [[22L 8s]] | |||
| [[22L 9s]] | |||
| [[22L 10s]] | |||
| [[22L 11s]] | |||
| [[22L 12s]] | |||
|- | |||
| [[23L 1s]] | |||
| [[23L 2s]] | |||
| [[23L 3s]] | |||
| [[23L 4s]] | |||
| [[23L 5s]] | |||
| [[23L 6s]] | |||
| [[23L 7s]] | |||
| [[23L 8s]] | |||
| [[23L 9s]] | |||
| [[23L 10s]] | |||
| [[23L 11s]] | |||
| [[23L 12s]] | |||
|- | |||
| [[24L 1s]] | |||
| [[24L 2s]] | |||
| [[24L 3s]] | |||
| [[24L 4s]] | |||
| [[24L 5s]] | |||
| [[24L 6s]] | |||
| [[24L 7s]] | |||
| [[24L 8s]] | |||
| [[24L 9s]] | |||
| [[24L 10s]] | |||
| [[24L 11s]] | |||
| [[24L 12s]] | |||
|} | |||
=== Larger MOS scales === | |||
[[7L 34s]], [[9L 29s]], [[12L 29s]], [[12L 41s]], [[13L 14s]], [[14L 13s]], [[17L 14s]], [[25L 6s]], [[41L 12s]] | |||
== Variations == | == Variations == | ||
* [[MODMOS scales]] are derived from chromatic alterations of one or more tones of an MOS scale, typically by the interval of {{nowrap| L − s }}, the "chroma". | |||
* [[MODMOS scales]] are derived from chromatic alterations of one or more tones of an MOS scale, typically by the interval of {{nowrap|L | * [[Muddle]]s are subsets of MOS parent scales with the general shape of a smaller (and possibly unrelated) MOS scale. | ||
* [[Muddle | |||
* [[MOS cradle]] is a technique of embedding MOS-like structures inside MOS scales and may or may not produce subsets of MOS scales. | * [[MOS cradle]] is a technique of embedding MOS-like structures inside MOS scales and may or may not produce subsets of MOS scales. | ||
* [[Operations on MOSes]] | * [[Operations on MOSes]] | ||
| Line 176: | Line 660: | ||
== References == | == References == | ||
<references/> | <references /> | ||
[[Category:Math]] | [[Category:Math]] | ||