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I may have to ask a mathematician
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aruffo
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PostPosted: Mon Jun 11, 2007 1:56 pm    Post subject: I may have to ask a mathematician Reply with quote

The idea of "saturation" as a dimension of pitch continues to appeal to me. On the one hand, it's an easy explanation for the fact that middle octaves, being more saturated, are better identified; on the other hand, it describes the desaturated sound of a fuzz guitar. What I'm still not sure about is how to move around the harmonic lattice (which I've attributed to Mathieu, but I've since learned the lattice has been around for centuries).

The idea of a "scale" that moves not through semitones but through increasingly complex ratios, starting with fifths (1:3) and thirds (1:5), is sensible and appealing-- but how do you move through it? It's easy enough to slide from one semitone to another by mathematically increasing or decreasing the vibratory frequency, but how do you gradually change 1:2 to 1:3 without passing through a host of ugly ratios in between?
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paul-donnelly



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PostPosted: Tue Jun 12, 2007 3:27 am    Post subject: Reply with quote

Is moving around the scale by simple ratios directly related to saturation? If not, I don't really see an issue. If you're sliding from semitone to semitone you pass through an infinite number of ugly ratios, while also starting and ending on ugly ratios. Why is it then a problem to find ugly ratios between two purely tuned notes as well?

The big difficulty I'm having with your tonal cylinder is how you actually go about increasing the saturation of a pitch.

Saturation is a difficult concept for me because there are so many ways to make the fundamental more difficult to perceive. You can take power away from all the lower harmonics, leaving only closely spaced high ones. You can distribute power unevenly to imply a different fundamental (e.g. adding power to the second and fourth harmonics will sound like the octave relationship normally only obvious at the root). You can increase the number of non-harmonic tones to add confusion. And each one of these strategies has an infinite amount of variability in its implementation.

While it's fairly easy to come up with a way to calculate a tone's saturation, going the other way looks like a huge problem to me.

By way of contrast, color is very easy. As we have only three color receptors, any way you slice it gives you a three-dimensional field (ignoring the overlap between the red, green, and blue receptors in our eyes, anyway). You can take a brightness for each of the three colors and combine them into a single luminance value, have a hue value for your position in the spectrum, and then add in the mysterious saturation. In visual media, saturation is an easy process-of-elimination concept.

If the color you're working with excites the red and green receptors, adding some more to blue receptor desaturates. From there, you can shift your red and green levels a little to keep the hue in the right place, and Bob's your uncle. Although it's possible to create a color that requires you to increase the level of two receptors in order to desaturate it, it's still easy to do. Essentially, you add a "harmonic" (more light at a new wavelength) right in between those two receptors, and hit them both. In either case, you're adding only one "harmonic." For the situation in which only the middle-spectrum green receptor is excited, you do have to add two new "harmonics", but this is likewise obvious. Adding only one would change the hue but not the saturation.

Again, I'm mostly ignoring the physiology of the eye, as I don't think it's relevant. The important part is that saturation in color theory follows directly from the fact that we only detect three color ranges. Adding more light frequencies is irrelevant, because our eye will simply sum them (simplified! Overlap between receptors does enhance our color discrimination). If we could see ultra-violet light our color model would gain a dimension (probably another hue, but who knows? Ask a tetrachromat how she thinks of it).

But how can we translate that to pitch? Rather than having three receptors, we have a huge number of them. Our whole auditory bandwidth from 15 or 20 Hz up to 20 to 30 kHz, divided up in intervals of 300 cents or so. So 80ish (!Warning: here be back-of-the-envelope math!). How do we decide which of these 80 bands to put energy into when we want to desaturate a pitch?

EDIT:
tl;dr -- While desaturing a tone and a color are similar and similarly hairy in theory -- both pitches and colors come with infinite spectra of companions -- color is vastly simplified by the simplicity of our color perceptors. We can ignore the infinite number of wavelength combinations possible, and focus on how the affect only three types of cone cell. This boils down to a three-axis concept of color, which can easily be transformed into the HSV system. Note, it is impossible to take an HSV or RGB color and procure the exact combination of wavelengths that produced it! The best we can do is create a color that will achieve that effect.

Sound however is made immensely more hairy by having 70 or so more receptors! This suggests to me that any direct translation of the RGB or HSV system would need as many axes. I'm not prepared to say that there is no meaningful three axis system that we can use to rotate tones, but I am prepared to say that a direct translation will have quite a few axes. Probably one for overall SPL, one for saturation, and many, many, many for "hue" or chroma, as you might call it.

However, I do take heart in the fact that we can ignore some of the variety of pitch and focus on under 100 classes of pitch, corresponding to critical bands, and that no one has to work directly with their extreme variability. Making a computer work out a way to increase a tone's saturation in 80 variables whilst maintaining its character in most of them (preserving chroma and timbre) doesn't strike me as anything like a show-stopper. The main issue, as with color, is picking which frequencies exactly to use. In the visual realm we've settled on three colors to use for computer monitors, but they are far from producing true-to-life colors (some, such as cyan and emerald, are missing entirely). It's possible that similar imprecision (which I predict will be heard as "roughness" of tone) will be tolerable in audio.
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paul-donnelly



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PostPosted: Tue Jun 12, 2007 3:56 am    Post subject: Reply with quote

So it's less a question of how to come up with a less saturated color than it's a question of which one we should use.

Not how to rotate a tone, but which way to turn it. I'm not quite clear on whether new axes change the hue axis into a hue space, or whether they create more concepts like "hue" and "value."


Assuming I'm right, you might want to glance at some stuff on 4 dimensional space. It can make the murky water of greater-than-3 dimensional rotation a little less murky. in 4D space, you get two (I believe) additional axes of rotation, which translate to some slightly incomprehensible motions when you move at right angles to the plane's we're used to.


Last edited by paul-donnelly on Tue Jun 12, 2007 4:16 am; edited 1 time in total
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TS



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PostPosted: Tue Jun 12, 2007 4:14 am    Post subject: Reply with quote

The ratios are due to how the harmonic overtones of single tones fit together.

Here's an article that explains it:
http://eceserv0.ece.wisc.edu/~sethares/consemi.html
And here's the original paper with more details:
http://eceserv0.ece.wisc.edu/~sethares/papers/consance.html

The infinite octave was about moving from 1:1 to 2:1, and that was accomplished by amplifying the harmonics that the 2:1 tone had, and diminishing the harmonics that the 1:1 tone had, so perhaps what is needed to move from 1:1 to 3:2 (perfect fifth) is to amplify the harmonics of the 3:2 tone, and diminish the harmonics of the 1:1 tone. Some harmonics will gradually disappear, some new ones will appear, and some will stay the same because they appear both in the 1:1 tone and the 3:2 tone.
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paul-donnelly



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PostPosted: Tue Jun 12, 2007 4:18 am    Post subject: Reply with quote

TS wrote:
The ratios are due to how the harmonic overtones of single tones fit together.

Here's an article that explains it:
http://eceserv0.ece.wisc.edu/~sethares/consemi.html
And here's the original paper with more details:
http://eceserv0.ece.wisc.edu/~sethares/papers/consance.html

The infinite octave was about moving from 1:1 to 2:1, and that was accomplished by amplifying the harmonics that the 2:1 tone had, and diminishing the harmonics that the 1:1 tone had, so perhaps what is needed to move from 1:1 to 3:2 (perfect fifth) is to amplify the harmonics of the 3:2 tone, and diminish the harmonics of the 1:1 tone. Some harmonics will gradually disappear, some new ones will appear, and some will stay the same because they appear both in the 1:1 tone and the 3:2 tone.

That's a viable method, I suppose. Less a shift than a fade, but akin to the way you would go from one color to another.
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aruffo
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PostPosted: Tue Jun 12, 2007 2:31 pm    Post subject: Reply with quote

Quote:
We can ignore the infinite number of wavelength combinations possible, and focus on how the affect only three types of cone cell. This boils down to a three-axis concept of color, which can easily be transformed into the HSV system.

This is what was initially hanging me up, but it's not quite on target. That is, the three-cone-cell definitely does translate into RGB or CMY(K, if you include rods), and I was assuming that HSV was the same-- but HSV is not a primary-color system. H is an infinite spectrum based on ordinal values; it's not a combination of primaries. The three axes of RGB and CMY are all essentially color values; in HSV, only one axis is color. (I wonder if "axis" should be in quotes because it's a circle?)

Quote:
While it's fairly easy to come up with a way to calculate a tone's saturation, going the other way looks like a huge problem to me.

I initially thought so too, and for the same reason-- too many receptors. What helped it makes sense to me is the progression of "pure tone" to "white noise", reading about the bagpipe's power spectrum, and hearing the fuzz guitar. With a color you add its complement to de-saturate. With a tone you add "noise".

The fact that there are "so many ways to make the fundamental more difficult to perceive" doesn't bother me because no matter how you do it, the result can boil down to a saturation value and a specific point within the cylinder. The interesting mathematical experiment would be, I think, if you somehow created the same functional point using different methods of desaturation; would they sound the same by virtue of their mathematical "saturation" value, or would they sound different because of the structural difference? I'd be inclined to think the former, but it'd have to be tested to be sure.

Quote:
perhaps what is needed to move from 1:1 to 3:2 (perfect fifth) is to amplify the harmonics of the 3:2 tone, and diminish the harmonics of the 1:1 tone. Some harmonics will gradually disappear, some new ones will appear, and some will stay the same because they appear both in the 1:1 tone and the 3:2 tone.

I thought maybe something like this would do the trick... but tho' I haven't yet tested it, I'm skeptical that it would work. The initial progression of intervals would be 1:1 to 1:2 to 2:3, or 1:2 to 2:3 in case the unison is less experimentally perceptible as an interval. The immediate theoretical problem I have with this kind of fusion is that, well, consider moving from 2:3 to 5:4. Once you have both a perfect fifth and a major third in relation to the root tone, aren't you necessarily creating a triad (and the minor third to go with it)?

For that matter, how do you get from 1:1 to 1:2?
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paul-donnelly



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PostPosted: Tue Jun 12, 2007 3:57 pm    Post subject: Reply with quote

aruffo wrote:
This is what was initially hanging me up, but it's not quite on target. That is, the three-cone-cell definitely does translate into RGB or CMY(K, if you include rods), and I was assuming that HSV was the same-- but HSV is not a primary-color system. H is an infinite spectrum based on ordinal values; it's not a combination of primaries. The three axes of RGB and CMY are all essentially color values; in HSV, only one axis is color. (I wonder if "axis" should be in quotes because it's a circle?)

HSV is a fairly simple transformation of RGB though. The fact that is has only three axes depends pretty directly on the fact that we started with only three.

Quote:
I initially thought so too, and for the same reason-- too many receptors. What helped it makes sense to me is the progression of "pure tone" to "white noise", reading about the bagpipe's power spectrum, and hearing the fuzz guitar. With a color you add its complement to de-saturate. With a tone you add "noise".

But fuzz boxes don't add white noise. They clip the wave down to a square wave, like the bagpipe, which is made up of the fundamental and all it's odd integer harmonics. The problem with simply adding noise is that we're so good at filtering out noise. It's going to sound like a tone and some noise up until the tone gets lost, not like an unsaturated tone. I think it will be necessary to be more subtle, but I can't put my finger on how.

Color is a lot simpler, since there are only three and there is no implied root, as in sound. Add some white to a color and it gets a little whiter. Add some white to a noise, and unless the added sound has some relationship to the fundamental, it sounds like an entirely new sound.

Quote:
The immediate theoretical problem I have with this kind of fusion is that, well, consider moving from 2:3 to 5:4. Once you have both a perfect fifth and a major third in relation to the root tone, aren't you necessarily creating a triad (and the minor third to go with it)?

For that matter, how do you get from 1:1 to 1:2?

Why is this a theoretical problem? Is there some reason that a triad shouldn't be temporarily created by that shift?

And what's the difficulty in doing octaves? Wouldn't you fade out the root while fading in the 1:2 interval?
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aruffo
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PostPosted: Tue Jun 12, 2007 7:56 pm    Post subject: Reply with quote

Quote:
But fuzz boxes don't add white noise. They clip the wave down to a square wave, like the bagpipe, which is made up of the fundamental and all it's odd integer harmonics.

I don't think we're disagreeing-- rather, I'm revealing my ignorance about this kind of process and terminology. I should learn to be more precise. If a fuzz box added white noise rather than altered the tone, then it would rightly, as you point out, be noise-plus-tone and not a desaturation.

I'm suggesting that "saturation" is something very much like the fuzzbox actually does do-- manipulate the harmonics of a tone so that they either support or detract from the fundamental frequency. The logical ends of such a continuum would be the presence of only octaves (27.5, 55, 110, 220, 440, etc) versus the presence of every possible tone at equal power (white noise).

Color is a helpful analogy only to a point, mainly because it is only an analogy. The fact that you can add white to a color and have it "get whiter" is, in my proposal of "saturation", comparable not to adding full-on white noise to a tone but increasing the power of all a tone's harmonics (perhaps especially the disconsonant ones?) so that the tone is perceptibly less pure while still recognizably possessing the same chroma.

Quote:
Why is this a theoretical problem? Is there some reason that a triad shouldn't be temporarily created by that shift?

The reason I'd give is that it would sound like a triad and not an ambiguous interval. I'll grant that when a chroma is slid along the infinite octave it tends to sound like an octave interval where the lower is "getting softer" while the higher is "getting louder", but played as discrete sounds the odd-height tones sound like individual tones, not octave intervals. When you play a C3.5 it sounds like a C which could be either C3 or C4; it doesn't sound like C3 and C4. If it is possible to move from a perfect fifth to a major third, it should be possible to create a sound which is somewhere "in between" the two, could potentially be either, but is still an interval (not a triad) which is perceptibly neither.
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paul-donnelly



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PostPosted: Tue Jun 12, 2007 11:44 pm    Post subject: Reply with quote

aruffo wrote:
I don't think we're disagreeing-- rather, I'm revealing my ignorance about this kind of process and terminology. I should learn to be more precise. If a fuzz box added white noise rather than altered the tone, then it would rightly, as you point out, be noise-plus-tone and not a desaturation.

I'm suggesting that "saturation" is something very much like the fuzzbox actually does do-- manipulate the harmonics of a tone so that they either support or detract from the fundamental frequency. The logical ends of such a continuum would be the presence of only octaves (27.5, 55, 110, 220, 440, etc) versus the presence of every possible tone at equal power (white noise).


All right; I'll buy that view. I think that's pretty much what I'm thinking as well: you've got to strengthen or add harmonics that ambiguate the tone.

aruffo wrote:
The reason I'd give is that it would sound like a triad and not an ambiguous interval. I'll grant that when a chroma is slid along the infinite octave it tends to sound like an octave interval where the lower is "getting softer" while the higher is "getting louder", but played as discrete sounds the odd-height tones sound like individual tones, not octave intervals. When you play a C3.5 it sounds like a C which could be either C3 or C4; it doesn't sound like C3 and C4. If it is possible to move from a perfect fifth to a major third, it should be possible to create a sound which is somewhere "in between" the two, could potentially be either, but is still an interval (not a triad) which is perceptibly neither.

This is sort of what was messing me up with the concept of adding noise. What do you do to create a tone with more noise rather than a tone and noise, and what do you do to fade from one interval to another rather than just playing both?
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aruffo
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PostPosted: Wed Jun 13, 2007 1:01 am    Post subject: Reply with quote

Quote:
what do you do to fade from one interval to another rather than just playing both?

If I still had Mathieu's book in hand I might have at least a better idea, but it disappeared in the mail last year (along with the rest of a box's contents). Mathieu has an exercise I wrote about on June 3, 2003 in which he illustrates the fifth and third "components" of a major seventh. I just tried the exercise again now-- I had to play the short tone clips on repeat so I could successfully drone along with them-- and I feel what I think he's referring to, but for some reason it's not the same "a-ha!" feeling it was back then (good heavens, was it four years ago already?).

I also looked at the rhythmic example immediately above which made me wonder... what would it look like if you simply combined the same kinds of dots? So I made this diagram (red is 2:3, green is 4:5, black is 8:15)

which, collapsed, looks like this

I'm not yet sure what can be drawn from this, though.
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TS



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PostPosted: Wed Jun 13, 2007 6:54 am    Post subject: Re: I may have to ask a mathematician Reply with quote

aruffo wrote:
What I'm still not sure about is how to move around the harmonic lattice (which I've attributed to Mathieu, but I've since learned the lattice has been around for centuries).

After thinking about it, I think that the middle point in the harmonic lattice triangle is a major chord.

I looked at the dissonance curve from the link I gave before and wondered why a major scale has a major 2nd and a major 7th degree, when according to this curve they form a dissonant interval with the root. Then I realised that they form consonant intervals with other tones of the scale.

So, the beginning point of the lattice is the root tone. You could add some consonant tones to the root (in this case the major 3rd and perfect 5th), and because these tones form a consonant interval with the root, they are a sort of a "decoration" on top of the root. The consonant tones do not change the root's identity to something else, they only add some tonal decoration to it, so that it sounds fuller and thicker.

Now you could fade out the root and the third, and leave only the fifth, and you would again have a single tone. And you could again add decoration to this single tone, by adding a major 3rd and a perfect 5th, but this time the added 3rd is to the original root a major 7th, and the added 5th is to the original root a major 2nd, so this is where the major 2nd and major 7th come to the major scale, and this is what the harmonic lattice is describing.
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aruffo
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PostPosted: Wed Jun 13, 2007 1:06 pm    Post subject: Reply with quote

Oh! That makes sense..! I like it especially since it continues to be a manipulation of overtones which means that it continues to be "pitch". I'll have to try that, both to see if I do in fact understand what you're describing and to see if it produces the desired effect.

I suppose I came near what you're describing when on the main page I came up with the tone which was 5% C-power; I just didn't take it all the way and fade out the C completely. In a way it already proves the point, because it's compositionally neither C nor E but could be perceptibly either.

A functional problem that I had had with that, and also with the problem of sliding along the infinite octave, is that where you start from determines the overtones immediately available to you. Once you move from C3 to C4, you can't move from C4 to C5 without introducing the C5's partials. However, once you fade in the C5's partials you can keep right along (which is exactly what I did to achieve the three-octave slide). So there must be something similar which can be done to move around the harmonic lattice-- even though fading from C to G means you don't have the G's partials immediately available to you, what you have is (in my current parlance) a somewhat desaturated G, and once you fade its partials in you can fade out the ones you need to remove to get to the next third or fifth.

The thing I'll be interested to find out, then, once I have a tone that is an acceptable midpoint between (as the best example) G and E-- does this, then, create an interval with the C-root which is ambiguously either a fifth or a third, without creating an interaction that is something entirely different?

If I find I can create a sliding harmonic interval space like this, I know exactly what experiment I want to conduct on it.
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paul-donnelly



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PostPosted: Thu Jun 14, 2007 4:11 am    Post subject: Reply with quote

This isn't 100% on-topic, but it follows from what we've been talking about: I just realized that I don't have the faintest idea why you're talking about harmonic lattices. Pardon me if you've written something on the topic already and I've forgotten or missed it (in which case a link would be wonderful), but I've never thought about lattices outside of a just intonation context, and the last time I checked you were primarily interested in the usual 12 tone equal tuning.
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PostPosted: Thu Jun 14, 2007 7:34 am    Post subject: Reply with quote

Hm... why am I talking about harmonic lattices? It's taken on somewhat a life of its own... I should check why I originally started paying attention to em and compare that with what I'm thinking about em now.

Oh yes. Once I started thinking that harmonic relative pitch was a more musically appropriate measure (and skill) than "distance" between intervals, I was pleased to encounter the lattice because it provided the alternative to the standard chromatic scale, describing how intervals could have harmonic rather than scale-step relationships.

The reason I've been wanting to move freely around the lattice space is that I want to find out if harmonic space is a legitimate continuum like the standard arithmetic scale, or if instead it's just a theoretical convenience.
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paul-donnelly



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PostPosted: Thu Jun 14, 2007 3:27 pm    Post subject: Reply with quote

aruffo wrote:
The reason I've been wanting to move freely around the lattice space is that I want to find out if harmonic space is a legitimate continuum like the standard arithmetic scale, or if instead it's just a theoretical convenience.

By "arithmetic scale" you mean the traditional Western 12 tone to the octave scale, right?
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