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{{Interwiki
|de=Delta-rationaler Akkord
|en=Delta-rational chord
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A '''delta-rational''' ('''DR''') chord is a [[chord]] that has integer ratios between frequency ''differences'' of some pair of intervals, called '''deltas''', with the intervals in question assumed to be between successive notes (Δ, capital delta, is often used to denote "difference").  
A '''delta-rational''' ('''DR''') chord is a [[chord]] that has integer ratios between frequency ''differences'' of some pair of intervals, called '''deltas''', with the intervals in question assumed to be between successive notes (Δ, capital delta, is often used to denote "difference").  


DR chords are a generalization of JI chords, in which all frequency differences of intervals are exactly integer ratios. But unlike JI chords, a DR chord need not have integer ratios between frequencies of notes. For example, the [[13edo]] chord {{dash|0, 3, 8, 10|med}}\13 ({{dash|, 277¢, 738¢, 923¢|med}}) is close to being delta-rational, because the frequency difference of the interval 8–10\13 is 0.994 times the frequency difference of the interval 0–3\13. (In the exactly DR chord {{dash|0\13, 3\13, 8\13, 924.159¢|med}}, the 3rd and 4th notes have exactly the same frequency difference as the interval 0–3\13.)  
DR chords are a generalization of JI chords, in which all frequency differences of intervals are exactly integer ratios. But unlike JI chords, a DR chord need not have integer ratios between frequencies of notes. For example, the [[13edo]] chord {{dash|0, 3, 8, 10|med}}\13 ({{dash|0{{c}}, 277{{c}}, 738{{c}}, 923{{c}}|med}}) is close to being delta-rational, because the frequency difference of the interval 8–10\13 is 0.994 times the frequency difference of the interval 0–3\13. (In the exactly DR chord {{dash|0\13, 3\13, 8\13, 924.159{{c}}|med}}, the 3rd and 4th notes have exactly the same frequency difference as the interval 0–3\13.)  


[[JI]] chords and chords that are subsets of [[Delta-rational chord#Isodifferential chord|isodifferential chord]]s (these correspond to all chords of the form α : {{nowrap|α + ''k''<sub>1</sub>}} : ... : {{nowrap|α + ''k''<sub>''n''</sub>}} for any positive (possibly irrational) number α and integers ''k''<sub>1</sub>, ..., ''k''<sub>''n''</sub>) are special cases of delta-rational chords, but in these chords ''all'' intervals are rationally related in frequency space, which we call '''fully delta-rational''' (FDR).
[[JI]] chords and chords that are subsets of [[Delta-rational chord#Isodifferential chord|isodifferential chord]]s (these correspond to all chords of the form α : {{nowrap|α + ''k''<sub>1</sub>}} : ... : {{nowrap|α + ''k''<sub>''n''</sub>}} for any positive (possibly irrational) number α and integers ''k''<sub>1</sub>, ..., ''k''<sub>''n''</sub>) are special cases of delta-rational chords, but in these chords ''all'' intervals are rationally related in frequency space, which we call '''fully delta-rational''' (FDR).
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We start by choosing the [[MOS scale]] and equave, and the DR chord.  
We start by choosing the [[MOS scale]] and equave, and the DR chord.  


For example with 5L 2s ⟨2/1⟩, the usual diatonic scale, and we want to approximate 4:5:6, the just major chord, with a delta-rational MOS chord.   
For example, with 5L&nbsp;2s, the usual diatonic scale, and we want to approximate 4:5:6, the just major chord, with a delta-rational MOS chord.   


Identify the mappings of each of the deltas. The deltas are 5/4, 6/5, 7/6. For a Meantone mapping, these are g<sup>4</sup>/4 -1, g-g<sup>4</sup>/4. This is because in meantone, 1/1, 3/2, 5/4 are 1, g, g<sup>4</sup>/4 respectively, so the deltas are identified by subtracting the each term with the one before it.  
Identify the mappings of each of the deltas. The deltas are 5/4, 6/5, 7/6. For a Meantone mapping, these are {{nowrap|''g''<sup>4</sup>/4 1}}, {{nowrap|''g'' − ''g''<sup>4</sup>/4}}. This is because in meantone, 1/1, 3/2, 5/4 are 1, ''g'', {{nowrap|''g''<sup>4</sup>/4}} respectively, so the deltas are identified by subtracting the each term with the one before it.  


In this case, we want the difference between our deltas to become 1, so the delta signature will be +1+1.  
In this case, we want the difference between our deltas to become 1, so the delta signature will be +1+1.  


To achieve this, we take the difference between the first two deltas and set it to zero, so (g<sup>4</sup>/4 -1) - (g-g<sup>4</sup>/4) = 0. Put in integer terms, it's g<sup>4</sup> - 2g - 2 = 0. Solving for g, the only root that makes sense is g≈1.49453, which in cents is 695.630c. And thus, with this generator, we will have a DR ~4:5:6 meantone chord!
To achieve this, we take the difference between the first two deltas and set it to zero, so {{nowrap|(''g''<sup>4</sup>/4 1) (''g'' − ''g''<sup>4</sup>/4) {{=}} 0}}. Put in integer terms, it's {{nowrap|''g''<sup>4</sup> 2''g'' − 2 {{=}} 0}}. Solving for ''g'', the only root that makes sense is {{nowrap|''g'' ≈ 1.49453}}, which corresponds to 695.63{{c}}. And thus, with this generator, we will have a DR ~4:5:6 meantone chord.


Note that the equation to solve depends on what chord you want to tune as equal-beating. For example, assuming pure octaves, Meantone admits an equation for tuning the 3:4:5 as equal-beating: {{nowrap|''g''<sup>4</sup> + 2''g'' − 8 {{=}} 0}} The latter equation has solution {{nowrap|''g'' {{=}} 1.4960 {{=}} 697.}}.  
Note that the equation to solve depends on what chord you want to tune as equal-beating. For example, assuming pure octaves, Meantone admits an equation for tuning the 3:4:5 as equal-beating: {{nowrap|''g''<sup>4</sup> + 2''g'' − 8 {{=}} 0}} The latter equation has solution {{nowrap|''g'' {{=}} 1.4960 {{=}} 697.3{{c}}}}.  


If instead we chose a Schismic mapping, the deltas would be g<sup>8</sup>/8 -1, 2/g - g<sup>8</sup>/8, which gives a generator of 498.308c for 4:5:6.  
If instead we chose a Schismic mapping, the deltas would be {{nowrap|''g''<sup>8</sup>/8 1}} and {{nowrap|2/''g'' − ''g''<sup>8</sup>/8}}, which gives a generator of 498.308{{c}} for 4:5:6.  


=== Mathematical definition ===
=== Mathematical definition ===
Let ''a'' and ''b'' be positive integers and suppose {{nowrap|gcd(''a'', ''b'') {{=}} 1}}. Let {{nowrap|''E'' &gt; 1}} be the frequency ratio of the equave. Consider a MOS ''a'''''L'''''b'''''s'''{{angbr|''E''}} with generator range <math>I \subseteq (1, \sqrt{E})</math> (in the linear frequency domain), and consider a pair ({{nowrap|'''u''', '''v'''}}) of notes from the root of a given triad in the MOS, {{nowrap|'''0''' (unison) &lt; '''u''' &lt; '''v'''}}. Let '''p''', '''g''' be a basis formally representing the MOS scale's period and generator. Write  
Let ''a'' and ''b'' be positive integers and suppose {{nowrap|gcd(''a'', ''b'') {{=}} 1}}. Let {{nowrap|''E'' &gt; 1}} be the frequency ratio of the equave. Consider a MOS ''a'''''L'''&nbsp;''b'''''s'''{{angbr|''E''}} with generator range <math>I \subseteq (1, \sqrt{E})</math> (in the linear frequency domain), and consider a pair ('''u''',&nbsp;'''v''') of notes from the root of a given triad in the MOS, {{nowrap|'''0''' (unison) &lt; '''u''' &lt; '''v'''}}. Let '''p''', '''g''' be a basis formally representing the MOS scale's period and generator. Write  


<math>\begin{align}
<math>\begin{align}
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The existence of an exact tuning for a delta signature specification is only guaranteed to hold when we only care about a ratio between ''two'' terms in the delta signature being exact. If we want to optimize an arbitrary specified delta signature (with some deltas possibly held free), we can use a least-squares-error solution instead to minimize the error.
The existence of an exact tuning for a delta signature specification is only guaranteed to hold when we only care about a ratio between ''two'' terms in the delta signature being exact. If we want to optimize an arbitrary specified delta signature (with some deltas possibly held free), we can use a least-squares-error solution instead to minimize the error.


== Least-squares error ==
== Error measures ==
Least-squares linear error (here linear means "in frequency space, not pitch space") is a proposed error measure for approximations to DR chords. Like any other numerical measure of concordance or error, you should take it with a grain of salt.
{{main|Error measures for DR chords}}
=== Fully DR ===
The idea motivating least-squares linear error on a chord as an approximation to a given delta signature is the following: Say we want the error of a chord 1:''r''<sub>1</sub>:''r''<sub>2</sub>:...:''r''<sub>''n''</sub> (in increasing order), with {{nowrap|''n'' &gt; 1}}, in the linear domain as an approximation to a fully delta-rational chord with signature {{nowrap|+δ<sub>1</sub> +δ<sub>2</sub> ... +δ<sub>''n''</sub>
}}, i.e. a chord
 
<math> x : x + \delta_1 : \cdots : x + \sum_{l=1}^n \delta_l.</math>
 
We can vary ''x'' and ask, "By at least how much (in the linear domain) does the approximating chord have to be off for any ''x'' > 0?" When a specific ''x'' > 0 achieves this minimum, the resulting chord with delta signature {{nowrap|+δ<sub>1</sub> +δ<sub>2</sub> ... +δ<sub>''n''</sub>
}} is taken to be the DR chord that is being approximated.
 
Rewriting a bit, suppose the chord that is considered the approximation is 1:''f''<sub>1</sub>:''f''<sub>2</sub>:...:''f''<sub>''n''</sub>. Let <math>D_i = \sum_{k=1}^i \delta_k</math> be the delta signature {{nowrap|+δ<sub>1</sub> +δ<sub>2</sub> ... +δ<sub>''n''</sub>
}} written cumulatively. Then the resulting linear least-squares optimization problem is
 
<math>
\displaystyle{ \underset{x}{\text{minimize}}  \sqrt{\sum_{i=1}^n \Bigg( \frac{x + D_i}{x} - f_i \Bigg)^2 }  = \underset{x}{\text{minimize}}  \sqrt{\sum_{i=1}^n \Bigg( 1 + \frac{D_i}{x} - f_i \Bigg)^2 } }
</math>
 
with solution
 
<math>
x = \displaystyle{\frac{\sum_{i=1}^n D_i }{-n + \sum_{i=1}^n f_i},}
</math>
 
which can be plugged back into the error formula to obtain the error. Note that scaling the delta signature does not affect the error, a critical property for a DR error measure.
 
The least-squares linear error measure does not form a metric on the set of delta signatures with a fixed number of terms, since it is not symmetric.
 
=== Partially DR ===
Suppose we wish to approximate a target delta signature of the form <math>+\delta_1 +? +\delta_3</math> with the chord <math>1:f_1:f_2:f_3</math> (where the +? is free to vary). By a derivation similar to the above, the least-squares problem is
 
<math>
\displaystyle {\underset{x,y}{\text{minimize}} \sqrt{\bigg(\frac{x + \delta_1}{x} - f_1 \bigg)^2 + \bigg(\frac{x+\delta_1 + y}{x} - f_2 \bigg)^2 + \bigg(\frac{x+\delta_1 + y + \delta_3}{x} - f_3 \bigg)^2 }}.
</math>
 
We can set the partial derivatives with respect to ''x'' and ''y'' of the inner expression equal to zero (since the derivative of sqrt() is never 0) and use SymPy to solve the system:
 
<syntaxhighlight lang="py">
import sympy
x = sympy.Symbol("x", real=True)
y = sympy.Symbol("y", real=True)
d1 = sympy.Symbol("\\delta_{1}", real=True)
d2 = sympy.Symbol("\\delta_{2}", real=True)
d3 = sympy.Symbol("\\delta_{3}", real=True)
f1 = sympy.Symbol("f_1", real=True)
f2 = sympy.Symbol("f_2", real=True)
f3 = sympy.Symbol("f_3", real=True)
err_squared = ((x + d1) / x - f1) ** 2 + ((x + d1 + y) / x - f2) ** 2 + ((x + d1 + y + d3) / x - f3) ** 2
err_squared.expand()
err_squared_x = sympy.diff(err_squared, x)
err_squared_y = sympy.diff(err_squared, y)
sympy.nonlinsolve([err_squared_x, err_squared_y], [x, y])
</syntaxhighlight>
 
We similarly include a free variable to be optimized for every additional +?, after coalescing two consecutive +?'s and omitting the middle note. If two variables are related to each other but not to the integer deltas in the signatures, they have a common variable.


== DR chords in small edos ==
== DR chords in small edos ==
=== Fully DR triads ===
=== Fully DR triads ===
{{main|Delta-rational triads in small edos}}
{{main|Delta-rational triads in small edos}}
=== Partially DR tetrads ===
=== Partially DR tetrads ===
{{main|Partially delta-rational tetrads in small edos}}
{{main|Partially delta-rational tetrads in small edos}}


== DR and RTT ==<!--Essentially tempered [[Dyadic chord|dyadic]] triads are also more difficult to tune with simple delta-signatures, since they lack simple JI preimages.-->
== DR and RTT ==<!--Essentially tempered [[Dyadic chord|dyadic]] triads are also more difficult to tune with simple delta-signatures, since they lack simple JI preimages.-->
As stated above, one can tune a rank-2 regular temperament or a MOS scale in such a way that a triad of interest exactly "inherits" its delta signature from a simple JI mapping.
As stated above, one can tune a rank-2 regular temperament or a MOS scale in such a way that a triad of interest exactly "inherits" its delta signature from a simple JI mapping.


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! rowspan="2" | Edos
! rowspan="2" | Edos
|-
|-
! g<sup>10</sup>
! ''g''<sup>10</sup>
! g<sup>9</sup>
! ''g''<sup>9</sup>
! g<sup>8</sup>
! ''g''<sup>8</sup>
! g<sup>7</sup>
! ''g''<sup>7</sup>
! g<sup>6</sup>
! ''g''<sup>6</sup>
! g<sup>5</sup>
! ''g''<sup>5</sup>
! g<sup>4</sup>
! ''g''<sup>4</sup>
! g<sup>3</sup>
! ''g''<sup>3</sup>
! g<sup>2</sup>
! ''g''<sup>2</sup>
! g<sup>1</sup>
! ''g''<sup>1</sup>
! g<sup>0</sup>
! ''g''<sup>0</sup>
|-
|-
|  
|  
Line 1,198: Line 1,151:
! colspan="2" rowspan="2" | Not JI, but isodifferential
! colspan="2" rowspan="2" | Not JI, but isodifferential
| style="white-space: nowrap;" | φ:(φ + 1):(φ + 2):(φ + 3)
| style="white-space: nowrap;" | φ:(φ + 1):(φ + 2):(φ + 3)
| rowspan="7" | No, not all or none
| rowspan="8" | No, not all or none
| +1+1+1
| +1+1+1
|-
|-
Line 1,243: Line 1,196:


== External links ==
== External links ==
* [https://inthar-raven.github.io/delta/ Inthar's DR chord explorer (Includes least-squares linear error calculation)]
* [http://turbofishcrow.github.io/delta/ Inthar's DR chord explorer (Includes least-squares linear error calculation)]


[[Category:Chords]]
[[Category:Chord]]
[[Category:Harmonic]]
[[Category:Harmonic]]
[[Category:Lists of scales]]
[[Category:Lists of scales]]
[[Category:Xenharmonic series]]
[[Category:Xenharmonic series]]

Latest revision as of 10:03, 13 April 2026

A delta-rational (DR) chord is a chord that has integer ratios between frequency differences of some pair of intervals, called deltas, with the intervals in question assumed to be between successive notes (Δ, capital delta, is often used to denote "difference").

DR chords are a generalization of JI chords, in which all frequency differences of intervals are exactly integer ratios. But unlike JI chords, a DR chord need not have integer ratios between frequencies of notes. For example, the 13edo chord 0 – 3 – 8 – 10\13 (0 ¢ – 277 ¢ – 738 ¢ – 923 ¢) is close to being delta-rational, because the frequency difference of the interval 8–10\13 is 0.994 times the frequency difference of the interval 0–3\13. (In the exactly DR chord 0\13 – 3\13 – 8\13 – 924.159 ¢, the 3rd and 4th notes have exactly the same frequency difference as the interval 0–3\13.)

JI chords and chords that are subsets of isodifferential chords (these correspond to all chords of the form α : α + k1 : ... : α + kn for any positive (possibly irrational) number α and integers k1, ..., kn) are special cases of delta-rational chords, but in these chords all intervals are rationally related in frequency space, which we call fully delta-rational (FDR).

Delta-rational chords provide a non-JI-based approach to concordance, since chords that are delta-rational with simple ratios between intervals (when measured as absolute frequency differences) tend to be perceived as more concordant than other chords. This acoustic effect is thought to be caused by synchronized interference beating among the fundamentals and among lower harmonics of the fundamentals; the effect may be more or less pronounced depending on register, timbre, the complexity of the linear relationship, etc. For example, the delta-rational acoustic effect is expected to be weaker in chords with wider voicings, as well as chords played in timbres with loud higher harmonics (because the higher harmonics would make the delta-rational relationships less obvious). The justification for only considering intervals between adjacent notes is that the resulting notes within the intervals could psychoacoustically interfere with the beating of the intervals.

Inversions and revoicings of DR chords may not be DR, unlike the case with JI chords where inversions and revoicing of JI chords stay JI. However, unlike the case with most JI chords, a 2/1-equivalent MOS scale can tune a DR chord exactly, provided that the chord's delta signature specifies two integer entries.

Denoting a delta-rational chord

Delta signature

A delta-rational chord is determined by two things:

  • The interval formed by its lowermost two notes;
  • Its delta signature which has integer ratios, i.e. a list of (scaled) frequency increases between successive notes, their ratios showing the simple rational relationships, with a + before each increase. Note that it is whether the deltas are rationally related to each other that defines DR, not whether the deltas are related to the frequency of the root. If we divide every term by the first term to make the first term 1, the result is called a normalized delta signature.
    • Fully delta-rational chords always have a delta signature with no irrational ratios between terms.
  • Two delta signatures are equivalent if one can be obtained from the other by scaling by a positive real number. For example, +2+e+3 is equivalent to +2φ+eφ+3φ, and both signatures imply a delta-rational chord.

For example, a chord with a +1+2+1 delta signature is a:(a + 1):(a + 3):(a + 4) for some possibly irrational a.

Deltas that are free, i.e. not required to be related to any other deltas are indicated with +?. For example, saying that a tetrad is "+1 +? +1" means the first two notes and the last two notes have almost equal frequency difference (thus the ratio between the differences is 1/1), but the middle two notes are not in any simple relationship with the two outer intervals. The example 13edo chord is approximately +1 +? +1.

If you have some sets of deltas related to each other but not to other sets of increments, you could write the related sets with variables a, b, c or use one fewer letter by writing one set with positive integers without variables: an +a +b +a +b chord can also be written +1 +c +1 +c where c = b/a.

Mathematical definitions

  1. A chord α1:...:αn is delta-rational (DR) or partially delta-rational (PDR) when the chord has two distinct intervals αk1k2 and αk3k4, such that αk1 < αk2 < αk3 < αk4 and (αk2 − αk1)/(αk4 − αk3) is rational. Equivalently, a chord is delta-rational if it has a delta signature with some integers showing up.
  2. When all intervals are linearly related, equivalently when the chord has a delta signature with all entries integers, we call the chord fully delta-rational (FDR).
  3. A chord that has a delta signature with all entries +1 is called isodifferential or linear.

Due to the aforementioned equivalence of delta signatures under scaling, delta signatures of n terms are really elements of [math]\displaystyle{ S^{n-1}; }[/math] this is because they are specifically in the subset that is the image of the all-positive orthant of [math]\displaystyle{ \mathbb{R}^n. }[/math]

In practice these terms can loosely refer to approximations of mathematically exact PDR and FDR chords, for example in edo tunings.

Finding a tuning of a MOS scale with an exact DR chord

Layman guide

We start by choosing the MOS scale and equave, and the DR chord.

For example, with 5L 2s, the usual diatonic scale, and we want to approximate 4:5:6, the just major chord, with a delta-rational MOS chord.

Identify the mappings of each of the deltas. The deltas are 5/4, 6/5, 7/6. For a Meantone mapping, these are g4/4 − 1, gg4/4. This is because in meantone, 1/1, 3/2, 5/4 are 1, g, g4/4 respectively, so the deltas are identified by subtracting the each term with the one before it.

In this case, we want the difference between our deltas to become 1, so the delta signature will be +1+1.

To achieve this, we take the difference between the first two deltas and set it to zero, so (g4/4 − 1) − (gg4/4) = 0. Put in integer terms, it's g4 − 2g − 2 = 0. Solving for g, the only root that makes sense is g ≈ 1.49453, which corresponds to 695.63 ¢. And thus, with this generator, we will have a DR ~4:5:6 meantone chord.

Note that the equation to solve depends on what chord you want to tune as equal-beating. For example, assuming pure octaves, Meantone admits an equation for tuning the 3:4:5 as equal-beating: g4 + 2g − 8 = 0 The latter equation has solution g = 1.4960 = 697.3 ¢.

If instead we chose a Schismic mapping, the deltas would be g8/8 − 1 and 2/gg8/8, which gives a generator of 498.308 ¢ for 4:5:6.

Mathematical definition

Let a and b be positive integers and suppose gcd(a, b) = 1. Let E > 1 be the frequency ratio of the equave. Consider a MOS aL bsE with generator range [math]\displaystyle{ I \subseteq (1, \sqrt{E}) }[/math] (in the linear frequency domain), and consider a pair (uv) of notes from the root of a given triad in the MOS, 0 (unison) < u < v. Let p, g be a basis formally representing the MOS scale's period and generator. Write

[math]\displaystyle{ \begin{align} \mathbf{u} &= u_p \mathbf{p} + u_g \mathbf{g} \\ \mathbf{v} &= v_p \mathbf{p} + v_g \mathbf{g} \end{align} }[/math]

as elements of [math]\displaystyle{ \mathbb{Z}^2\langle \mathbf{p}, \mathbf{g}\rangle }[/math].

Define the rational function [math]\displaystyle{ r_{\mathbf{u}, \mathbf{v}} : I \to (0,\infty) }[/math] by

[math]\displaystyle{ \displaystyle{r_{\mathbf{u}, \mathbf{v}}(x) = \frac{E^{v_p}x^{v_g}- E^{u_p}x^{u_g}}{E^{u_p}x^{u_g} - 1} }. }[/math]

Then, provided that the positive rational number [math]\displaystyle{ m/n }[/math] lies in the image [math]\displaystyle{ r_{\mathbf{u}, \mathbf{v}}(I) }[/math] and [math]\displaystyle{ m(E^{u_p}x^{u_g} - 1) = n(E^{v_p}x^{v_g}- E^{u_p}x^{u_g}) }[/math] yields a nondegenerate polynomial equation after cancelling negative powers, we can solve for the frequency ratio [math]\displaystyle{ g \in I }[/math] that satisfies [math]\displaystyle{ r_{\mathbf{u}, \mathbf{v}}(g) = m/n, }[/math] making the specified chord (0, u, v) a + n + m DR chord.

The existence of an exact tuning for a delta signature specification is only guaranteed to hold when we only care about a ratio between two terms in the delta signature being exact. If we want to optimize an arbitrary specified delta signature (with some deltas possibly held free), we can use a least-squares-error solution instead to minimize the error.

Error measures

DR chords in small edos

Fully DR triads

Partially DR tetrads

DR and RTT

As stated above, one can tune a rank-2 regular temperament or a MOS scale in such a way that a triad of interest exactly "inherits" its delta signature from a simple JI mapping.

Below is a list of temperaments and their various optimizations for proportionally beating chords. They are ordered by highest power in the relevant DR polynomial, with ties broken by leading coefficients, then 2nd term coefficients, 3rd term coefficients, 4th term coefficients, etc. In the case of negative coefficients, only the absolute value is considered.

Coefficients of terms Chord Delta signature Temperament Generator (cents) Edos
g10 g9 g8 g7 g6 g5 g4 g3 g2 g1 g0
1 −1 −1 4:5:6 +1+1 [1 -2 1 833.09 (φ) 36
2 −1 −2 4:5:6 +1+1 Father 428.42 14
3 −2 −2 6:7:9 +1+2 Beep 258.65 33, 42, 51
1 −1 −2 4:5:6 +1+1 Mavila 523.66 23, 39
1 −2 −2 4:5:6 +1+1 Meantone 695.63 19, 31, 50
1 2 −4 4:5:6 +1+1 Porcupine 160.89 15
1 −4 12 5:6:9 +1+3 Mavila 674.90 16, 25
1 −4 −4 4:5:6 +1+1 Avila 660.23 20
1 −2 2 4:5:6 +1+1 Hanson 317.96 19
1 −2 −4 4:5:6 +1+1 Uncle 467.46 18
3 −4 −16 4:5:7 +1+2 Mabila 527.66 25
1 −1 −1 4:5:6 +1+1 Tetracot 176.54 34
1 −1 −4 4:5:6 +1+1 Sensi 442.74 19, 65
1 2 −8 4:5:6 +1+1 Orson 271.51 22, 31, 53

Higher-order differences of frequency

Generalizing, one could consider chords where differences between its frequency deltas (as Tom Price has called them, precessions) are rationally related, while the deltas themselves may not be. This corresponds to chords where differences between various interference beatings go in and out of sync in a periodic manner. One precession-rational chord is 5:5.4142...:6.8284...:9.2426..., a +(√2 − 1) +√2 +(√2 + 1) chord.

Precession being the second-order difference (δ2) of frequency, we similarly have the theoretical notions of δ3-rationality, δ4-rationality, and so on. The practical consequences of higher-order differences are as of yet speculative, though a few people have reported finding precession psychoacoustically meaningful.

Isodifferential chord

In an isodifferential chord (known variously by linear chord, equal-hertz chord, equal-beating chord, and proportional-beating chord), the frequencies of the pitches are in an arithmetic sequence, or in other words, there is an equal difference in cycles per second between successive pitches.

Isoharmonic chord

An isoharmonic chord is a specific type of isodifferential chord, where the ratios between the notes are rational numbers, and therefore the chord is in just intonation. Such a chord can be built by successive jumps up the harmonic series by some number of steps. Since the harmonic series is arranged such that each higher step is smaller than the one before it, all isoharmonic chords have this same shape—with diminishing step size as one ascends.

An isoharmonic "chord" may function more like a "scale" than a chord (depending on the composition of course), or even a series in the sense of a harmonic series, but the word "chord" is used here for consistency.

Classification

Class I

The simplest isoharmonic chords are built by stepping up the harmonic series by single steps (adjacent steps in the harmonic series). Take, for instance, 4:5:6:7, the harmonic seventh chord. We may call these class I isoharmonic chords. There is one class I series (the harmonic series), which looks like this:

Harmonic 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16
Cents diff 1200 702 498 386 316 267 231 204 182 165 151 139 128 119 112

Some "scales" built this way: otones12-24, otones20-40...

Class II

The next simplest isoharmonic chords are built by stepping up the harmonic series by two (skipping every other harmonic). This gives us chords such as 3:5:7:9 (the primary tetrad in the Bohlen–Pierce tuning system) and 9:11:13:15. Note that if you start on an even number, your chord is equivalent to a class I harmonic chord: 4:6:8:10 = 2:3:4:5. Thus, there is one class II series (the series of all odd harmonics):

Harmonic 1 3 5 7 9 11 13 15 17 19 21 23 25 27 29 31
Cents diff 1902 884 583 435 347 289 248 217 193 173 157 144 133 124 115
Class III

Class III isoharmonic chords are less common and more complex sounding. They include chords such as 7:10:13:16 and 14:17:20:23. Note that if you start on a number divisible by three, you'll again get a chord reducible to class I (e.g. 9:12:15 = 3:4:5). There are two series for class III:

Harmonic 1 4 7 10 13 16 19 22 25 28 31 34 37 40 43 46
Cents diff 2400 969 617 454 359 298 254 221 196 176 160 146 135 125 117
Harmonic 2 5 8 11 14 17 20 23 26 29 32 35 38 41 44 47
Cents diff 1586 814 551 418 336 281 242 212 189 170 155 142 132 122 114

Some "scales" built this way: 11:14:17:20...

Class IV
Harmonic 1 5 9 13 17 21 25 29 33 37 41 45 49 53 57 61
Cents diff 2786 1018 637 464 366 302 257 224 198 178 161 147 136 126 117
Harmonic 3 7 11 15 19 23 27 31 35 39 43 47 51 55 59 63
Cents diff 1467 782 537 409 331 278 239 210 187 169 154 141 131 122 114
Class V
Harmonic 1 6 11 16 21 26 31 36 41 46 51 56 61 66 71 76
Cents diff 3102 1049 649 471 370 306 259 225 199 179 162 148 136 126 118
Harmonic 2 7 12 17 22 27 32 37 42 47 52 57 62 67 72 77
Cents diff 2169 933 603 446 355 294 251 219 195 175 159 146 134 125 116
Harmonic 3 8 13 18 23 28 33 38 43 48 53 58 63 68 73 78
Cents diff 1698 841 563 424 341 284 244 214 190 172 156 143 132 123 115
Harmonic 4 9 14 19 24 29 34 39 44 49 54 59 64 69 74 79
Cents diff 1404 765 529 404 328 275 238 209 186 168 153 141 130 121 113

Notation

Some complex isoharmonic chords can be expressed with an offset from a simpler isoharmonic chord, so it is useful to notate them in a compact and readable way. For example, 41:51:61 is very similar to 4:5:6, so it can be notated as (4:5:6)[+0.1]. Similarly, (20:22:24:27:30:33:36)[+0.339] can be expanded to 20339:22339:24339:27339:30339:33339:36339.

Irrational isodifferential chords can be expressed with the same notation by using irrational numbers within the square brackets. For example, the chord (1:2:3)[+φ] can be expanded to (1 + φ):(2 + φ):(3 + φ), which is approximately equal to 1.618:2.618:3.618.

Categorization of DR chords

Here is a table which uses the "delta ratio set"–the set of unique undirected ratios between the deltas of a chord's delta signature–to categorize chords.

  • How to tell a DR chord from a non-DR chord: a DR chord has at least one rational number in its delta ratio set.
  • Within DR chords, how to tell an FDR chord from a non-fully DR chord: a FDR chord has only rational numbers in its delta ratio set.
  • Within FDR chords, how to tell an isodifferential chord from a non-isodifferential chord: an isodiffential chord has only 1 in its delta ratio set.

All JI chords are FDR chords, because JI chords are rational, and therefore their delta ratio sets will include only rational numbers.

If an FDR chord is both JI and isodifferential, then it is an isoharmonic chord.

Chord type Illustrative examples
Actual chord Deltas Delta ratio set
Frequency ratio Are items all integers? Delta signature Reduced delta signature (class) Are items all the same? Unique undirected ratios between the deltas Are items all rational?
DR FDR JI, not isodifferential 4:5:7:8 yes, all +1+2+1 +1+2+1 no, not all {1, 2} yes
3:5:9:11 +2+4+2
3:4:7:9 +1+3+2 +1+3+2 {3/2, 2, 3}
Isoharmonic
(JI and isodifferential)
Class I 4:5:6 +1+1 +1+1 Yes, all {1}
4:5:6:7 +1+1+1 +1+1+1
3:4:5:6
Class II 3:5:7:9 +2+2+2
5:7:9:11
Class III 1:4:7:10 +3+3+3
2:5:8:11
... ... ...
Not JI, but isodifferential φ:(φ + 1):(φ + 2):(φ + 3) No, not all or none +1+1+1
1:φ:(2φ − 1):(3φ − 2) +(φ − 1)+(φ − 1)+(φ − 1)
Not JI or isodifferential φ:(φ + 1):(φ + 3) +1+2 +1+2 no, not all {2}
(Incompletely) DR 4:5:τ:7:9 +1+(τ − 5)+(7 − τ)+2 +1+(τ − 5)+(7 − τ)+2 (irrelevant for categorization) {(7 − τ)/(τ − 5), 7 − τ, τ − 5, 2/(τ − 5), 2, 2/(7 − τ)} no, but at least one
5:τ:8:(3 + τ) +(τ − 5)+(8 − τ)+(τ − 5) +1+(8 − τ)/(τ − 5)+1 {1, (8 − τ)/(τ − 5) }
1:(1 + a):(1 + a + b):(1 + a + 2b):(1 + 3a + 2b),
with a/b irrational
+a+b+b+2a +a+b+b+2a {a/b, 1, 2, 2a/b}
Not DR 4:5:τ:7 +1+(τ − 5)+(7 − τ) +1+(τ − 5)+(7 − τ) {(7 − τ)/(τ − 5), 7 − τ, τ − 5} No, none
5:τ:7 +(τ − 5)+(7 − τ) +1+(7 − τ)/(τ − 5) {(7 − τ)/(τ − 5)}

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