Friday, November 24, 2023

Distance Measurements in OP-Space: Mapping tensional profiles

Comparing the discussion on geometric distances in Julian Hook’s new book Exploring Musical Spaces (2023) and the Dmitri Tymoczko classic A Geometry of Music (2011), we can see that there’s been quite the development on geometric distance research in the twelve-ish years between the two monographs. The main point of uncertainty still lies, however, in what ways we can measure the distance between two nodes in any geometric representation of musical space. I will try to explore the options in this post.

Let us look at the ways to measure the distance between sets of pitches in OP-space, since this is the basis of my current research. There should be no difference between using OP-space or any combination of OPTIC spaces. I have chosen to use OP-space since it most easily models individual chords without quality equivalence or inversion equivalence. Therefore, it is possible to model aural perceptions of tonal and post-tonal words closely, since our understanding of harmony allows octave equivalence and honestly, permutation equivalence exists to make my life easier, without thinking about choral inversions. It closely models the Lewinian transformational system that came before it, and this new model will have some of the same limitation as transformational models will too. A new post will come upon the completion of this paper.

Three main ideas are touched upon in the Hook (2023) and two ideas (overlapping with the Hook) in the Tymoczko (2011), to measure distance based on either the maximum distance in one voice, the Euclidian distance between the two nodes, or the ‘taxicab’ distance, the distance that follows the voice leading pathway between the two nodes.

Distance measurement ideas (reproduced from Hook 2023):



And the accompanying figure (Figure 12.4.1):



So, what works the best? Tymoczko (2011), in the appendix, talks about how not one measurement works better than another measurement, and it just depends on what the theorist is measuring for. Therefore, let us use his definition and apply it to this paper. For this paper, I am measuring distance to determine tensional profiles, so let us try all three ways of measuring distance and determine which one best suits our ears in determining the tensional relationships between chords. For our test, let us move away from a two-voice graph, as we have in the figure above, and move to a three-voice graph, as shown below (Figure 11.3.4 in the Hook 2023), to hear the relationships between triads, and not dyads:



Since this graph depicts all three voice triad combinations, related by semitonal voice leading, any combination of three notes fits onto this graph neatly, and most important to our test, it can be measured to determine the distance between any two nodes. It is important to note that this three-dimensional graph is no different than the two-dimensional graph above in the reproduced Figure 12.4.1, the node (alpha and beta) containing the three voices of the chord (Xn, Yn, and now with the addition of the third voice, Zn) are all the exact same in both versions and function the same as well. This graph just contains every single three voice combination, so we can calculate chords and collections aside from major and minor chords. This will be useful in the future, but just not for our upcoming example. When we perform the calculations based on the three methods above, we do the same in the two voiced version and the three voiced version.

 

Analysis of a real-life example

Let us take an example from John Adams’ Nixon in China, Act II, Scene 1, from Pat’s Aria “This is prophetic”. The first six chords are as follows:

Eb minor à B7 dominant à Eb minor à E major à E minor à C major

Let us further skip over the four-note chord, B7 dominant for now, since cross-types are a whole other topic, better discussed at length elsewhere. We shall simplify the B7 into a B major chord, eliminating the seventh.

Then we can calculate the distances between all the chords in this progression based on our three methods shown above. First let’s just number our chord relationships for ease:

Eb minor [1] B (major) [2] Eb minor [3] E major [4] E minor [5] C major

And to keep our OP-space, we shall accept octave equivalence and permutations of the chord (any order of voices in our set), so we will seek the smoothest voice leading, as according to the three-voice graph above. And thus:

distMAX:

[1] 1

[2] 1

[3] 2

[4] 1

[5] 1

 

distEuc:

[1] 1

[2] 1

[3] sqrt (6)

[4] 1

[5] 1

 

distVL:

[1] 1

[2] 1

[3] 4

[4] 1

[5] 1

An interesting pattern is formed! The chords that share two common tones, and thus the ones that can be modelled with basic Neo-Riemannian transformations, relation [1, 2, 4, 5], agree in all three systems. They are separated by one semitone. Since these relationships [1, 2, 4, 5] maps onto transformations [L, L, P, L] is it obvious that they share two common tones and therefore the distance between them is the one tone that moves by semitone. Relation three [3], however, is what we’re interested in. In the voice leading distance, it measures Eb minor to E major as 4 semitones of distance, in the Euclidian, square root of 6 (~2.45) semitones, and in the ‘maximum’ calculation, 2 semitones. If we put it in Neo-Riemannian terms, it is a parallel transformation, a SLIDE transformation, and another parallel transformation, P-SLIDE-P.

 

So, which distance calculation is the best (for this analysis)?

What shall we use? Hook (2023) says that most theorists choose to use the voice leading calculation in their work, since it most closely models what we hear. I agree with that. It closely follows the path that the voices need to travel to reach the next chord. It also models Neo-Riemannian transformations very well, since each movement in the voice leading space corresponds to a basic Neo-Riemannian transformation, so it is just like chaining basic transformations together.

If we go the Euclidian path, it also makes some sense. Since it is a straight line in our perfectly organized space, the distance is the shortest path to get from one chord to the next.

The maximum distance does not seem to work well with what we are looking at. Since it is a simplification of the voice leading relationships by only looking at the voice that moves the furthest, it neglects to model situations where the other two (or more) voices are moving lesser amounts, but not holding common tones. Therefore, if we have a chord that holds common tones and a chord that does not, the maximum distance calculation will not make a difference.

The solution is to combine some aspects of the voice leading calculation, for it seems to model the way that the notes travel naturally in our ears, while using the Euclidian path to model distances in the full phrase. In our example above then, the chords that ‘sound’ next to each other, like Eb minor to B (major), will be analyzed using the voice leading distance, since they are truly voice leading from one to the next. But when looking at the distance travelled from Eb minor (first chord) to C major (last chord), since these two chords are not sounding next to each other, we will use the Euclidian path, as it is the straight path to measure the overall distance travelled in a phrase (or whole section). We can then get the best of both worlds without sacrificing musical logic!

 

Issues

Certain issues come up with this analysis. First, there is a difference between OP- and O-space. The fact that the chords are permutable, and I can find the most parsimonious path between the chords means that we are not really measuring the voice leading in this section, but rather the perfect world where the voices go very smoothly. In the above example, the chords are actually rather choppy. This will be expanded upon in the future, where I fine tune this thesis to fit the music a bit better.

The second issue was touched upon very briefly before. How do we do the cross type? How do we move from three notes to four notes? We will, as I said before, discuss this in a later post.

The third issue comes when we get the distance numbers. When graphed, these relationships are just numbers that rise and fall according to the relationship between the chords. But if we wanted to see how the whole phrase functions, in what way can we manipulate this data to give us the ‘mode’ of the rising and falling distance? Should we also calculate the distance between the first chord and every other chord? Should we look at how close the phrase is to tonal ideas and map it that way? Many avenues are still to be explored in the next post.


No comments:

Post a Comment