Concept

Unison — where it appears

Two or more sources sounding what is meant to be one pitch. Nothing about it is trivial: a piano's three strings are deliberately a cent or two apart for the sustain, and a choir's sixteen are fifteen cents apart because people are, which is what makes a section sound like a section.

Named by 13 essays across 5 fields — each of them below, with the objects they name alongside it.

The fluctuation stays; the rate goes. A unison of n voices with a spread of 15 cents, averaged over 5 draws. The depth of the amplitude fluctuation does not fall as voices are added — a choir is no steadier than a duet — but the fraction of that fluctuation in any single modulation component falls from 77 per cent at two voices to 24 at 32. Two voices make one beat and it can be counted; 16 make 120 and none of them is a rate. That is why a choir cannot be tuned by nulling anything.

What a choir does that a soloist cannot

Two singers on one note produce one beat and it can be counted. Sixteen produce a hundred and twenty at once, and the amplitude still fluctuates by as much as it did — a choir is no steadier than a duet. What has gone is not the fluctuation but its rate: the modulation energy that sat in a single line at two voices is spread across a band at sixteen, with no line in it. That is the choral sound, and it is also why the just-intonation drift measured for tuned singing describes only ensembles that hold their pitch still.

timbre · The voice
One pair, 12 beat rates. Two notes at 220 hertz, 15 cents apart, drawn as the beat rate between each pair of partials. The fundamentals beat at 1.91 hertz and the k-th partials at k times that, so the series of rates is a straight line and it crosses 15 hertz at the 8th partial. Below the line the fluctuation is counted; above it the same physical fluctuation is heard as roughness. 1 per cent of this spectrum's energy is on the roughness side. The bars are drawn at each partial's own amplitude, so a spectrum with little energy high up crosses the line where nothing is listening.

Every partial beats at its own rate

Five earlier essays have drawn one beat rate per figure, and every one of them is the rate between two fundamentals. Two real notes beat between all of their partials at once, the k-th pair beats k times as fast, and somewhere up the spectrum the rate passes the point at which a beat stops being a beat — so a chorused note is a beat at the bottom of itself and a roughness at the top, simultaneously, with a crossover partial that is arithmetic.

tuning · Beating
Which interval gives a tuner the deepest null. A tuner listening to an interval p:q is listening to the lower note's p-th partial against the upper note's q-th, and how deep the beat's trough goes is decided by those two amplitudes rather than by the interval. For a string spectrum, whose partials fall as one over n, the minor third pairs partial 6 against partial 5 at a ratio of 1.18 for a dip of 21.8 decibels; the major third pairs partial 5 against partial 4 at a ratio of 1.25 for a dip of 19.1 decibels; the fourth pairs partial 4 against partial 3 at a ratio of 1.32 for a dip of 17.2 decibels; the fifth pairs partial 3 against partial 2 at a ratio of 1.52 for a dip of 13.8 decibels; the major sixth pairs partial 5 against partial 3 at a ratio of 1.65 for a dip of 12.2 decibels; the minor sixth pairs partial 8 against partial 5 at a ratio of 1.67 for a dip of 12.0 decibels; the octave pairs partial 2 against partial 1 at a ratio of 2.00 for a dip of 9.5 decibels. The best is the minor third at 21.8 and the worst is the octave at 9.5, which is the reverse of the order a tuner is usually taught to trust: the deepest null in the list is on the interval whose coincidence sits highest in the spectrum, where adjacent partials are nearly equal in strength.

A beat has a depth, and six essays held it at one

Every beat figure so far adds two tones of equal amplitude, which is the single ratio at which the trough of a beat is a true null — and a null is what a tuner is actually listening for. Vary the ratio and the picture changes: at two to one the dip is nine and a half decibels, at ten to one it is under two, and the interval that gives the shallowest null of all is the octave.

intervals · Beating
Where a section's fluctuation stops being a beat, on 220 hertz. Two rates up the spectrum of a 220 hertz note sung by a section whose voices are spread by 15 cents. The rising line is the beat rate between a typical pair of them, which grows with the partial because a mistuning in cents is a difference in hertz that scales with frequency; it reaches the 15 hertz at which a beat stops being a beat by partial 5.5, at 1217 hertz. The flat line is the amplitude modulation the vibrato imposes through the formants, which is 6.0 hertz at every partial because the vibrato modulates every partial by the same number of cents at the same rate. The two are equal at 487 hertz. Above 1217 hertz the beating has become roughness and the only fluctuation left is the vibrato's — and that frequency is the same one an octave up, where it is partial 2.8 instead.

The rate that does not rise with the partial

Twelve earlier essays give every vibrato the same six hertz, and the measured spread is 5.5 to 7.5. Putting the two fluctuations a choir contains on one axis shows why the rate matters: the beating between mistuned voices rises with the partial and leaves the range a listener follows as fluctuation at 1,217 hertz, while the vibrato's own modulation is six hertz at every partial. Above that frequency a section fluctuates by vibrato alone — and if every singer had the same rate, it would barely fluctuate at all.

instruments · The voice
14 players summed, against the one at their average onset. Each thin line is one player's rising envelope, started at its own moment, with a spread of 30 milliseconds about the beat and a 90-millisecond attack. The heavy line is the section: nominally identical sources add incoherently, so their powers add and the sum is the root of the mean of their squares, drawn here as a fraction of the section's own peak. The dashed line is the single player who started at the section's average onset. The section reaches the 6 dB below peak criterion at 18.1 milliseconds and that player at 27.6, a difference of 9.5. The section is early because the players who started first are already sounding while the average one is still building, and nothing a late player does can make the sum quieter.

Twelve violins are more punctual than one

Every essay until now treats a part as one player, and an orchestral part is a dozen. Sectioning does two things at once and only one of them was expected: it pulls the part's heard moment forward, by four milliseconds against a map spanning twenty-six, and it makes the part's arrival more accurate by very nearly the root of the number of players. So the map of required leads applies to an orchestra better than it applies to a quartet, and the case where it fails is three trumpets rather than fourteen violins.

rhythm · Perceptual-centre
How wide the unison is left decides how far down the aftersound starts. A two-string unison on A3, each string decaying in 20 seconds alone and the pair's bridge-driving mode in 1.5, struck and heard at the bridge, against how many cents apart its strings are tuned: the drop from the prompt sound to the aftersound, for a hammer that strikes both strings alike and for one that strikes the second 20 and 50 per cent softer. Even strike: 0.25 cents 65.2 dB, aftersound 19.9 s; 0.5 cents 53.1 dB, aftersound 19.5 s; 1 cent 41.0 dB, aftersound 18.0 s; 1.5 cents 33.7 dB, aftersound 16.0 s; 2 cents 28.4 dB, aftersound 13.8 s; 2.5 cents 24.2 dB, aftersound 11.6 s; 3 cents 20.5 dB, aftersound 9.7 s; 4 cents 13.8 dB, aftersound 6.5 s; 5 cents 6.3 dB, aftersound 4.0 s. The earlier count assumed 20 dB; the unison gives that at about three cents. At a perfect unison the aftersound is not excited at all, and past 5.33 cents the two modes split and the unison beats instead. A strike's force scales both modes alike and appears nowhere in the drop.

The octave is counted best over a unison left two and a half cents wide

A firm touch buys a mistuned octave's beats only if the aftersound's drop does not deepen with the strike, and the drop was left as a number to be measured. It has a mechanism, and the mechanism has been known since the essay on three strings: the unison's two coupled modes. Computed from them, the drop does not depend on the strike at all. It depends on how wide the tuner left the unison — sixty-five decibels at a quarter of a cent, twenty at three — and the octave's beats peak, at 6.8, over the same two-and-a-half-cent unison that makes the longest note.

intervals · Beating
Where the tilt of the blow matters, and where it does not. The octave's beats at 80 dB against the tilt of the blow from the vertical: one string, others muted, 0° 2.81, 1° 2.81, 2° 2.81, 3° 2.81, 5° 2.81, 8° 2.87, 12° 3.19, 16° 3.62, 20° 4.27; a unison half a cent wide, 0° 1.51, 1° 1.51, 2° 1.51, 3° 1.51, 5° 1.57, 8° 1.95, 12° 2.60, 16° 4.00, 20° 4.87; a unison 2.5 cents wide, 0° 6.81, 1° 6.81, 2° 6.81, 3° 6.81, 5° 6.87, 8° 6.87, 12° 6.70, 16° 6.97, 20° 7.25. One string alone and a clean unison both get their aftersound from the second plane and both gain beats as the blow tilts. The wide unison already has an aftersound twenty-odd decibels down from its own detuning, and the second plane, at forty, adds nothing it can hear.

The plane of the blow matters only where the unison is clean

A piano string vibrates in two planes, and the one parallel to the soundboard gives even a single string a second, slower decay. A hammer tilted off the vertical feeds it. That was the last way left for a firm touch to cost a tuner beats: if harder blows came down straighter. They would have to straighten by half for every seven decibels, and even then only on a single string or a unison tuned clean. Over a unison left two and a half cents wide, no tilt of the blow reaches the count.

intervals · Beating
A vibrato hides a section's beats above about four hundred hertz. Two voices of a section whose tuning is spread by 15 cents, singing one note: how many nulls of their beating a listener can follow each second — counted only while the beat is at or below fifteen a second — at the frequency of the partial compared, sung straight and with a 71-cent vibrato at about six hertz. 220 Hz 2.2 straight, 5.3 with vibrato; 330 Hz 3.3 straight, 4.4 with vibrato; 440 Hz 4.2 straight, 3.9 with vibrato; 550 Hz 5.0 straight, 3.3 with vibrato; 660 Hz 5.1 straight, 2.8 with vibrato; 880 Hz 5.5 straight, 2.4 with vibrato; 1100 Hz 4.8 straight, 2.0 with vibrato; 1320 Hz 4.6 straight, 1.5 with vibrato; 1760 Hz 3.9 straight, 1.2 with vibrato; 2200 Hz 3.5 straight, 1.1 with vibrato; 2640 Hz 3.2 straight, 0.9 with vibrato; 3200 Hz 2.3 straight, 0.7 with vibrato; 3520 Hz 2.0 straight, 0.7 with vibrato. Below 413 hertz the vibrato adds followable beats, because it sweeps a slow difference faster. Above it the vibrato removes them, because it carries the pair's difference past fifteen hertz most of the time; at 3,200 hertz, the singer's formant, a straight section gives 3.4 times as many.

A vibrato hides a choir's tuning above four hundred hertz

Thirteen essays drew a vibrato that had always been running; a real one grows out of a straight tone over the first quarter-second of a note. Counting the beats a listener can follow between two voices of a section shows what that front edge is worth. A vibrato takes most of a section's countable beats away above about 400 hertz — seven in ten of them at the singer's formant — and adds some below. The straight start gives them back only while the vibrato is still growing, and in the band where a voice carries that is less than one beat.

instruments · The voice
A section's vibratos must lock almost completely before its tuning is exposed again. Two voices of a section spread by 15 cents, each with a 71-cent vibrato near six hertz, their vibratos pulled together so that their differences of rate and phase shrink to a stated share: followable beats a second at three partial frequencies, against how far they are locked, with the same voices sung straight as the dashed line beside each. 660 Hz (straight 5.14): 0 2.77, 0.25 2.90, 0.5 3.23, 0.7 3.85, 0.8 4.45, 0.85 4.98, 0.9 5.02, 0.95 5.31, 0.98 5.17, 1 5.15; 1217 Hz (straight 4.66): 0 1.60, 0.25 1.80, 0.5 2.04, 0.7 2.58, 0.8 2.88, 0.85 3.29, 0.9 3.88, 0.95 4.41, 0.98 4.67, 1 4.66; 3200 Hz (straight 2.33): 0 0.68, 0.25 0.70, 0.5 0.80, 0.7 1.13, 0.8 1.10, 0.85 1.45, 0.9 1.70, 0.95 1.98, 0.98 2.12, 1 2.23. At the singer's formant, half-locked vibratos expose 34 per cent of what a straight section does, locked to nine-tenths 73 per cent, locked to ninety-five 85 per cent; only at about ninety-eight per cent does it come within a tenth of a straight section.

A choir's vibratos must lock to two milliseconds

A vibrato hides a section's mistuning from a listener counting beats, and the obvious way it could stop hiding it is for the singers' vibratos to move together. They would have to move very nearly together. Half-entrained vibratos leave a section as hidden at the singer's formant as independent ones; locked to nine-tenths they expose three-quarters of what a straight section does; only past nineteen parts in twenty does the section's tuning show as if they sang straight. At six cycles a second that is two vibratos peaking within two milliseconds of each other — and the better a section is tuned, the tighter the lock has to be.

instruments · The voice
Heard a little late, two vibratos lock in step; heard a third of a cycle late, they lock in opposition. Two singers' vibratos at 6.0 and 6.2 a second, each pulled towards the phase it hears from the other with a strength of 10 radians a second, the hearing delayed by a stated time: how far apart the two vibratos' peaks settle, in milliseconds, after twenty seconds. 0 ms: 1.6 apart (4°); 20 ms: 2.4 apart (5°); 40 ms: 61.9 apart (-169°); 60 ms: 70.7 apart (-176°); 80 ms: 79.5 apart (-176°); 100 ms: 88.1 apart (-176°); 120 ms: 95.7 apart (-175°); 140 ms: 1.6 apart (4°); 160 ms: 1.6 apart (4°); 180 ms: 1.8 apart (4°); 200 ms: 69.6 apart (-176°). Under about forty milliseconds the lock is near in phase; from about forty to a hundred and twenty it is near antiphase, the peaks most of half a cycle apart; from about a hundred and forty, nearly a whole cycle late, it is near in phase again. The shaded band is the two milliseconds the formant asked for.

Singers who hear each other late lock their vibratos in opposition

A choir's vibratos give back the section's tuning at the singers' formant only if they are locked to within about two milliseconds. Singers who lock do it by hearing each other, and they hear each other late. Two vibratos pulled towards what each hears of the other settle near in step while the delay is under about forty milliseconds, and even then come within two milliseconds only if each singer corrects a phase error in about thirty. From forty to a hundred and twenty milliseconds late — a third to two-thirds of a vibrato cycle — they lock in opposition, peaks seventy to ninety milliseconds apart, and hide the section's tuning more completely than vibratos that never locked at all.

instruments · The voice
Where a pair would lock in opposition, a section of sixteen does not lock at all. Sixteen singers in two rows of eight, sixty centimetres apart, each hearing every other after the sound's travel and a common latency, each vibrato pulled towards all it hears with a total strength of 10 radians a second; four draws of rates and phases. Against the latency: R1, the length of the mean of the vibratos' phases, one when every vibrato is in step; and R2, the same for twice the phases, one also when the section has split into two opposed halves. 0 ms: 0.96, 0.86; 10 ms: 0.94, 0.83; 20 ms: 0.89, 0.71; 30 ms: 0.72, 0.52; 40 ms: 0.47, 0.31; 50 ms: 0.09, 0.24; 60 ms: 0.07, 0.22; 70 ms: 0.08, 0.23; 80 ms: 0.08, 0.22; 90 ms: 0.10, 0.24; 100 ms: 0.19, 0.22; 110 ms: 0.68, 0.46; 120 ms: 0.90, 0.73; 135 ms: 0.96, 0.85; 150 ms: 0.97, 0.87. A section split in two would show R2 high with R1 low; it never does.

Sixteen singers cannot all oppose each other

Two singers who hear each other a third of a vibrato cycle late lock their vibratos in opposition and hide their tuning better than if they had not listened at all. Sixteen cannot do it, because no arrangement puts every one of them opposite every other. At the latencies where a pair opposes, a section of sixteen does not lock at all: each singer keeps a vibrato rate of its own, and a listener hears the section's tuning exactly as through independent vibratos. Outside that band the section locks in step and gives most of its tuning back. A section that listens to itself can expose its tuning or leave it as it was, but never hide it.

instruments · The voice
A row that hears its neighbours late hides the tuning between them, exposes it between every second singer, and leaves the whole as it was. Sixteen singers in one row sixty centimetres apart, a draw of fifteen cents apart with 71-cent vibratos, each pulled at ten radians a second towards what it hears, each voice's pull weighted by the inverse of its distance to the power 8; four draws. The beats a second a listener can follow at 3,200 hertz, against the latency, for neighbouring pairs, for pairs two places apart, and over every pair. neighbours: 0 ms 1.62, 20 ms 1.36, 40 ms 0.69, 60 ms 0.30, 80 ms 0.28, 100 ms 0.29, 120 ms 0.78, 150 ms 1.63; every second singer: 0 ms 1.23, 20 ms 0.90, 40 ms 0.82, 60 ms 0.94, 80 ms 1.21, 100 ms 1.15, 120 ms 0.90, 150 ms 1.21; every pair: 0 ms 0.96, 20 ms 0.77, 40 ms 0.72, 60 ms 0.67, 80 ms 0.67, 100 ms 0.69, 120 ms 0.75, 150 ms 0.92. Sung straight 2.33, independent vibratos 0.68, a pair in opposition 0.19.

A row that hears its neighbours moves its tuning, it does not hide it

Sixteen singers who all hear each other alike cannot lock in opposition, because opposition between every pair is impossible. A row that hears mainly its neighbours has no such obstacle — opposition along a chain is consistent — and at the latencies that make a pair oppose, it half-alternates: neighbours opposite each other, every second singer nearly in step. That hides the tuning between neighbours as well as a duet hides it, and exposes it between every second singer more than independent voices would. Over the whole row the two cancel to the hundredth. With no latency, the same local hearing stops the row locking at all, and hides nearly half of what a whole-row lock would show.

instruments · The voice
Two strings a few cents apart carry the pair through every interval the regulator feared, and its brightness breathes. A harpsichord's two eight-foot registers, plucking at 32 and 50 millimetres from the nut of a 355-millimetre string, each on its own string of a unison at C5, the second tuned 2 cents above the first: the spectral centroid of the pair, in partial numbers, through the first three seconds of a note (both strings decaying alike). At the pluck it is the aligned pair's 2.44; through the note it ranges from 2.29 to 3.67, repeating every 1.65 seconds. The detuning carries the pair past the regulation tolerance of a decibel at the fundamental — 0.153 of a period — after 254 milliseconds (the line). Every half second: 0.0 s 2.44, 0.5 s 3.12, 1.0 s 3.34, 1.5 s 2.53, 2.0 s 2.90, 2.5 s 3.66, 3.0 s 2.89.

Two strings undo what two quills were regulated for

A harpsichord's two eight-foot registers each pluck their own string of a unison, and the unison is never exact. Two cents apart, the second string's partials turn against the first's at a rate proportional to their number, so within a quarter of a second at C5 the pair has drifted past the regulation tolerance the jacks were voiced to, and through the rest of the note it passes again and again through every interval a regulator could have set. The pair's fixed spectrum becomes one that breathes, its own holes become flickers a few per cent of a cycle long, and averaged over the note the second register is worth a decibel and a half at the fundamental, not four.

instruments · Excitation point

Named alongside it

The objects these essays reach for when they reach for this one.

BeatingModulationVibratoFormantPartialRoughnessTuning by earChorus effectCoupled oscillatorCritical bandwidthDecayHammer

All concepts