Stems and cones

Where a handover sits

Inside every rung there is a rise at which the two contact steps change places, so that the shorter hop belongs to the other family below it. Six of the eight rungs on this ladder have one, each has exactly one, and every one of them sits in the coarse half.

Worth reading first: Counting the spirals · A head is a set of points · The rung was not the instrument.

A rung is a range of rises over which a counter, shown nothing but the point positions, returns one pair of numbers. That constancy is the whole of what the word means, and it is why the ladder is the useful picture of this subject: the counts do not slide, they step.

Inside a rung, though, things move. The settled divergence slides. The front deepens. And there is a third quantity, which this essay is about, that not only moves but reverses: which of the two contact families has the shorter step.

The golden ladder, rung by rung. Each bar is one rung — a run of rises over which a counter returns one pair — drawn from its coarse end on the left to its fine end on the right, with the whole bar scaled to the same width so that positions inside different rungs can be compared. The mark on each bar is the rise at which the two contact steps change places, and it falls between 12 and 35 per cent of the way down on every rung that has one. The dots are the lattices this collection's ablation census was grown at, dropped onto the rungs they belong to. They are not spread across the bars; seven of them sit past the mark.
Fig. 1 Each bar is one rung, scaled to a common width, with the rise at which the two steps change places marked on it.

What the two steps are

Take a stem at a settled divergence and a rise. Every pair of organs k places apart is joined by a step that runs some way around the cylinder and some way up it, and the length of that step is a number the lattice fixes. Rank the lags by that length and the first two are, by definition, the contact families — the two numbers a counter returns.

Which offsets give short hops, at a rise of 0.013. The two lowest points are at 5 and 8, and those are the parastichy numbers. Offset 1 is high because a hop of one node is at least the rise, which is what makes a stem easier to count than a disc.
Fig. 2 The lengths of the steps at every lag, on one lattice, with the two shortest picked out.

Which of those two is first is a separate question from which two they are, and it is a question nothing in a count answers. A stem counted at five and eight spirals can have the five-step shorter or the eight-step shorter, and a counter returns five and eight either way.

Which offsets give short hops, at a rise of 0.018. The two lowest points are at 5 and 8, and those are the parastichy numbers. Offset 1 is high because a hop of one node is at least the rise, which is what makes a stem easier to count than a disc.
Fig. 3 The same ranking at the coarse end of the same rung, where the shorter of the two belongs to the other family.
Which offsets give short hops, at a rise of 0.008. The two lowest points are at 5 and 8, and those are the parastichy numbers. Offset 1 is high because a hop of one node is at least the rise, which is what makes a stem easier to count than a disc.
Fig. 4 And near its fine end, where they have changed places again.

So somewhere inside the rung the two lengths are equal, and the ordering changes hands there. Call that rise the rung’s handover. It is not a place where anything visible happens: no count changes, no front changes width, nothing about a drawing of the stem looks different. It is a place where a ranking swaps.

Six of eight, and each exactly once

The ladder here carries eight rungs between rises of 0.0040 and 0.0700 — four on the golden branch and four on the Lucas one. Measured by sweeping the rise at one per cent and reading the hop ranking at each step, six of the eight have a handover inside the range, and each of those six has exactly one.

The Lucas ladder, rung by rung. Each bar is one rung — a run of rises over which a counter returns one pair — drawn from its coarse end on the left to its fine end on the right, with the whole bar scaled to the same width so that positions inside different rungs can be compared. The mark on each bar is the rise at which the two contact steps change places, and it falls between 6 and 40 per cent of the way down on every rung that has one. The dots are the lattices this collection's ablation census was grown at, dropped onto the rungs they belong to. They are not spread across the bars; three of them sit past the mark.
Fig. 5 The Lucas branch, whose rungs carry handovers of their own at quite different places.

The two without one are the coarsest rung on each branch — golden 2/3 and Lucas 1/3 — and their absence is a statement about the range swept rather than about them. Both are cut off at 0.0700, which is as coarse as this collection’s stems go before the pattern stops being a lattice worth counting, and the arithmetic says their crossings sit above it.

That each of the six has exactly one is the part worth pausing on, because it is not obvious. Two lengths that cross could cross three times, or five. That they cross once is a consequence of the two curves involved being smooth and one of them being shallower than the other over the whole rung, which is an argument the arithmetic makes and no sweep needed to discover.

The plane of stems: divergence across, rise up. Each shade is one parastichy pair. The marked points are the lattices where three families are equally short — the forks — and the Fibonacci ones run up the middle towards 137.51°.
Fig. 6 The diagram the rungs come from, where each branch is a curve on which two families are equidistant and each node is a place three of them are.

How it was measured, and what would have broken it

The ranking is read from the ideal lattice rather than from a grown stem: at each rise the settled divergence is measured once, the step lengths of the first forty lags are computed from that divergence and that rise, and the list is sorted. That separation matters. A ranking read off a grown stem’s own neighbour graph would fold the rule’s noise into the answer, and near a handover the two lengths differ by parts in a thousand, so any noise at all would decide the ordering instead of the geometry.

A cell's neighbours are its spiral families. Left: part of a 700-point golden, 137.508° head, with every contact between two cells drawn and coloured by the difference between the two nodes' placement indices. Right: the share each difference takes, across all 1459 contacts between interior cells. They are the parastichy numbers — 34, 55, 21, 89, 13, 8 — and the pair a person would count is 34 and 55. The six sides Euler forces are shared out among four of them, 5.64 edges per cell.
Fig. 7 What a contact family is in the arrangement rather than in the ranking: the organs an organ actually touches.

Two things would have made the measurement worthless and neither happened.

The first is that a handover could have been an artefact of the azimuth grid. The divergence is quantised — a stem’s angles land on a grid of 1,536 steps — and if the two step lengths differ by a thousandth then a grid step of a quarter of a degree could easily be what decides which is shorter. Re-measured on a grid four times finer, the handovers move by less than one sweep step. They are in the geometry rather than in the discretisation.

The second is that the ranking could have been unstable — the two lengths crossing, recrossing and crossing again over a few rises, so that “the handover” was a region rather than a rise. It is not. On every rung the ratio of the second length to the first falls monotonically to one and rises monotonically away from it, which is the shape a single crossing has and not the shape a fluctuating ranking has.

The divergence slides along the 5/8 rung. Measured at every rise on one rung, where a counter returns 5 and 8 spirals throughout. The settled divergence slides from 136.6406 to 137.8672 degrees. The ratio of the two contact steps falls to 1.0131 at a rise of 0.016 and the ordering changes hands at 0.015: above it the shorter step belongs to the 5-family and below it to the 8-family. Neither quantity is available to a counter, which is shown positions and reports a pair, and both of them move while that pair does not.
Fig. 8 The settled divergence over the same rung, whose smooth slide is what makes the crossing single rather than repeated.

What remains is a bound rather than a defect: within about one per cent of a handover the two lengths differ by less than the ranking can meaningfully separate, so a rise landing there has no ordering worth quoting. That is not a failure of the measurement; it is what “equal” means when it is approached from both sides. It matters in practice, because one of the census’s own lattices sits within two and a half parts in a thousand of a handover, and the readings scored on that row have been quoting an ordering that is not there.

And every one of them is in the coarse half

Here is the measurement this essay exists for. Taking the position of a handover as a fraction of the way down its own rung from the coarse end — measured in the logarithm of the rise, because the ladder is geometric — the six sit at:

branch rung handover position
golden 3/5 12%
golden 5/8 15%
golden 8/13 35%
Lucas 3/4 40%
Lucas 4/7 6%
Lucas 7/11 33%
Where a rung's handover sits, over six rungs. The rise at which the two contact steps change places, as a fraction of the way down each rung from its coarse end, over every rung on both branches that has one. All six fall in the coarse half and none in the middle: the positions measure 6, 12, 15, 33, 35, 40 per cent. That is a fact about the arithmetic of the lattice rather than about any experiment run on it, because the crossing is where the two step lengths are equal and both are functions of the rise and the divergence alone.
Fig. 9 The same six positions as a distribution. All of them fall in the coarse half and none in the middle.

Six of six in the coarse half, spread from six per cent to forty. Never past the middle, and never at either end.

Six is a small number and it is worth being clear about what it can carry. The claim is not that a handover can never sit past the middle — nothing here proves that — but that on both branches of this ladder, over every rung the range reaches, it does not. Two branches with unrelated seed angles and pairs from 3/5 to 7/11 is a wider base than a single branch would be, and the arithmetic behind it is the same on any branch, which is the reason to expect the pattern to hold where it has not been checked rather than to assume it.

Why the coarse half

The handover is where the two step lengths are equal, and that condition defines a curve in the plane of rise against divergence: for each rise there is one divergence at which the two families are equidistant. The rule’s own settled divergence traces a second curve across the same rung.

Two lines across the 5/8 rung, crossing once. The divergence the rule settles on, against the divergence at which the two contact steps would be exactly the same length. The second is arithmetic on the lattice and no stem is grown for it. Across this rung the balanced line moves 2.281 degrees and the rule's own line moves 1.262, so the shallower line crosses the steeper one, and it does so exactly once at a rise of 0.0154 — 16 per cent of the way down from the coarse end. That crossing is the handover: above it one family has the shorter step and below it the other does. So a rung has one handover, its position is fixed by the arithmetic rather than by any experiment, and a sweep of the rise carries a stem across it at a place nobody chose.
Fig. 10 The two curves across one rung, and the single place they cross.

Across the 5/8 rung the balanced curve moves 2.281° and the rule’s own moves 1.262°, so the rule’s line is the shallower one. It starts above the balanced line at the coarse end, crosses it, and finishes below. Where it crosses depends on how the two slopes compare, and on this ladder the balanced line is consistently about twice as steep — which puts the crossing nearer the coarse end than the fine one, on every rung.

Two lines across the 4/7 rung, crossing once. The divergence the rule settles on, against the divergence at which the two contact steps would be exactly the same length. The second is arithmetic on the lattice and no stem is grown for it. Across this rung the balanced line moves 3.537 degrees and the rule's own line moves 2.602, so the shallower line crosses the steeper one, and it does so exactly once at a rise of 0.0222 — 7 per cent of the way down from the coarse end. That crossing is the handover: above it one family has the shorter step and below it the other does. So a rung has one handover, its position is fixed by the arithmetic rather than by any experiment, and a sweep of the rise carries a stem across it at a place nobody chose.
Fig. 11 The same pair of curves on the Lucas branch, where the divergence falls rather than rises and the crossing is nearer still to the coarse end.

So the answer to “why the coarse half” is arithmetic rather than biological or dynamical. It is a statement about the relative slopes of two curves, one of which is fixed by the lattice and one of which is where the placement rule settles.

What it is for

Two things, and the second is why it is worth an essay rather than a footnote.

The first is that a handover is a place to put a controlled experiment. Straddle it and the counted pair is held, the settled divergence is nearly held, and the step ordering flips — which is a matched comparison with one quantity varying, and it is exactly the design the ablation thread needed and had no way to state before the rung’s interior was mapped.

The two steps changing places inside the 5/8 band. Measured at every rise of a band on the golden branch, where a counter returns 5 and 8 spirals throughout. The settled divergence moves by 0.0469 degrees across the whole band, which is a fraction of the azimuth grid step and a fortieth of the slide across the rung it sits in. The ratio of the two contact steps does move: it falls to 1.0013 and the ordering changes hands at a rise of 0.0156, so above that rise the shorter step belongs to the 5 family and below it to the 8 family. Two of the three quantities that vary along a rung are therefore held here and the third is not, which is what makes the ends of this band a matched pair.
Fig. 12 The ordering crossing inside a band around one handover, where the divergence is held to a twentieth of a degree.

The second is that a handover explains a puzzle in the tables. Every census here grows one stem per rung, and the position that stem sits at was never recorded. Positioned now, eight of the ten lattices that produce a wrecked stem sit past their rung’s handover — which is not a coincidence but a consequence of this measurement. If a handover is always in the coarse half, then a rise picked anywhere near the middle of its rung is past it, and picking rises near the middle is what a person does when they want a rise that reliably produces a pair.

The column the census never carried. One row per lattice the ablation census was grown at. The bar shows where inside its own rung that rise sat, measured in the logarithm of the rise because the ladder is geometric, with zero the coarse transition and one the fine one. The mark on each bar is that rung's own handover, the rise where the two contact steps change places. Of the ten lattices that ever wreck, eight sit past their handover and one sit before it, with one sitting so close to one that the two steps differ by parts in a thousand. The rise was recorded in every table this collection has published; this fraction was in none of them.
Fig. 13 The census’s own lattices, each on its rung, with the handover marked.

That turns an accident of sampling into something predictable: any census built the sensible way, by anybody, will sit past the handover on nearly every row.

The name, and why it needed one

This collection has got along without a word for it until now, which is itself worth a paragraph. The quantity has been visible in the tables since the hop ranking was first computed — every ranking ever printed here has a first entry and a second — and the reversal was noticed once, in passing, as a thing that happens along a rung. It was not named, and unnamed quantities do not get measured across a ladder.

The consequence was concrete. The reading that a wrecked stem keeps its shortest hop was stated, scored and refuted without anybody establishing where the census sat relative to the reversal, because there was no noun to hang the question on. With one, the question asks itself: which side was each row on? That is the whole content of the next two essays, and neither needed a new experiment.

A wreck is a whole number of extra turns. For each of the 19 stems that never repair, the slip of its settled divergence multiplied by the lag whose hop survived. Every value lands on a whole number of turns — the horizontal lines — with a largest departure of 2.97 degrees, against divergences that have moved between 0 and 103 degrees. 17 of the 19 close on exactly one turn. So a wrecked stem is the stem it was with one extra turn threaded through every period of the family that survived, which is a dislocation with a stated size rather than damage.
Fig. 14 The census the reading was scored on, which carries a ranking in every row and never carried the side.

What a handover is not

It is not a transition. A transition is where the counted pair changes and the ladder steps; a handover is inside a rung and changes nothing a counter can report. Two rises either side of a transition are different lattices; two rises either side of a handover are the same lattice with its two nearest-neighbour families ranked the other way round.

Every transition as the rise falls. The pair climbs 1/2 → 2/3 → 3/5 → 5/8 → 8/13. Consecutive transitions are 0.381, 0.382, 0.382 of the previous rise — 1/φ² is 0.3820.
Fig. 15 The transitions, which are what the ladder is made of, and which the handovers sit between rather than at.

It is not a fork. A fork on the van Iterson diagram is where three families are equidistant, and those have a closed form and sit at exactly rational divergences. A handover has two families equidistant, which happens along a whole curve rather than at isolated points, and the rule crosses that curve once per rung.

The hops of a 5/8 lattice, shortest first — golden, rise 0.010Every lattice hop at this rise, ordered by how long its step is across the surface of the stem, with the two that a wrecked stem here leaves standing picked out. The two shortest are the contact families the counter returns, 5 and 8, and they differ in length by a factor of 1.076. The lags left standing after a removal are 5 and 8, sitting at rank 2 and 1 in this order, so the family the rule holds is a short step but not always the shortest one.85133161021181122624629lag, in organs — ordered by the length of its stepstep length, in turns of the stemkept: lag 5, lag 8golden, rise 0.010 · pair 5/8 · offsets that wreck: 4, 5, 6, 7, 8generated from a stated rule, not drawn to look right
Fig. 16 The hop ranking at one lattice, which is the object a handover reorders and a fork rebuilds.

And it is not, on the evidence so far, a place where the mechanism does anything. Cutting an organ out of a stem either side of a handover leaves the same family standing, at every offset that wrecks, on both bands measured. That is a negative result about the ablation rather than about the handover, but it does bear on how much weight the ordering should carry: a ranking that reverses without changing an outcome is a ranking the outcome does not depend on.

The ordering changes and the survivor does not. Every offset that wrecks, at every rise of the band, with the family left standing written in the cell. The counted pair is 5 and 8 at all 18 rises and the settled divergence is held to a twentieth of a degree, so the one quantity moving across the columns is which of the two contact steps is the shorter — and it changes hands at the marked rise. The cells do not: the 5 family survives at all 24 wrecked cuts, on both sides. Scored on this band, the reading that a wrecked stem keeps its shortest hop is right 14 times out of 24, for an answer that never changed.
Fig. 17 The ordering reversing across a band, with the family that survives written in every cell.

What a reader can check

The whole of this is arithmetic on two numbers, which makes it unusually easy to verify without any of the machinery here. Pick a rise, take the settled divergence at that rise, and compute for each lag k the horizontal offset — k times the divergence, folded to within half a turn and divided by a full one — and the vertical offset, k times the rise. The step length is the hypotenuse. Sort. The first two entries are the pair a counter will return, and which of them comes first is the ordering this essay is about.

The two spiral families a counter finds between 0.43 and 0.67 of the radius. 21 spirals one way and 34 the other, found from the point positions alone — the counter is never told the divergence angle.
Fig. 18 The counter that returns the pair, which is shown positions and never a divergence, and which cannot see the ordering at all.

Doing that at 0.018 and at 0.008 on the golden branch gives five first and then eight first, with the same pair reported both times. Doing it at a hundred rises in between finds exactly one place the order changes. That is the measurement, and it takes a spreadsheet.

The part that is not arithmetic is the settled divergence, which has to come from somewhere. Here it comes from growing a stem under the placement rule and averaging its last sixty divergences, which is the same measurement the rest of this collection uses and which carries the rule’s own choices with it. Substituting the ideal Fibonacci limit angle instead — 137.5077° at every rise — moves the handovers by several per cent of a rung and does not move any of them out of the coarse half. So the finding survives the substitution, and the substitution is worth naming because it is the one a reader is most likely to make.

six limit divergences, all of them 137.5078 over a whole number. The golden angle is the k = 1 member of a family. Real bijugate plants — teasel, Cephalaria — are reported near 68.75°, which is exactly half of it, and the pairs they are counted at are the Fibonacci pairs doubled.
Fig. 19 The limit angles a substitution would use, which are what the rule approaches rather than what it sits at.

What is left

The obvious extension is the rungs this range cannot reach. Both branches’ coarsest rungs have their crossings above 0.0700, and both branches stop below about 0.005 for a reason that has now been measured: a stem below that does not settle onto a lattice at any run length. So the six rungs here are not six of many available; they are six of eight, and the other two are outside the window rather than unexamined.

Which rises are a lattice, from 0.04 to 0.13. How much the divergence wanders over the last sixty organs, at each rise up the coarse ladder. 13 of the 19 settle, scattering between 0.0000 and 0.3356 degrees. six do not: from 0.09 to 0.115 the divergence sticks on exactly 135.0000 degrees, which is three eighths of a turn, and wobbles about it by 0.79 to 1.60 degrees. A counter shown either kind returns the same pair, so the counts cannot tell them apart. The line is the threshold a rise has to pass before a cut is made on it, and it sits in the gap rather than among the measurements.
Fig. 20 The coarse end of the ladder, where the two rungs without a measured handover live.

The more interesting extension is whether the position of a handover is predictable from the pair alone. Six positions is enough to notice that the coarse half is where they are and not enough to fit anything; the two rungs at six and twelve per cent carry pairs whose numbers are close together, and the two at thirty-five and forty carry pairs whose numbers are further apart. That could be a real relation or it could be four numbers arranged into a story, and the honest thing is to say which of those it is only after the arithmetic has been asked directly rather than the sweep.

The two contact steps change places inside the 5/8 rung. Measured at every rise on one rung, where a counter returns 5 and 8 spirals throughout. The settled divergence slides from 136.6406 to 137.8672 degrees. The ratio of the two contact steps falls to 1.0131 at a rise of 0.016 and the ordering changes hands at 0.015: above it the shorter step belongs to the 5-family and below it to the 8-family. Neither quantity is available to a counter, which is shown positions and reports a pair, and both of them move while that pair does not.
Fig. 21 The quantity a handover is the zero crossing of, drawn across one rung.

What links here

Computed from the collection, not written here: the essays that point at this one.

Reads more easily once this is understood

Essays that name this one as worth reading first.

Shares its objects with

Essays that name at least two of the same things, and that neither author linked.

  • What a count cannot decide — both name counting blind, contact network, divergence angle, lattice, measurement, parastichy, parastichy pair, rise, rung
  • A stem coarse enough to cut — both name counting blind, divergence angle, lattice, measurement, parastichy pair, rise, rung, transitions
  • A stem too fine to settle — both name counting blind, contact network, lattice, measurement, parastichy, parastichy pair, rise, rung
  • The ratio was the floor of a curve — both name divergence angle, ladder, measurement, nearest neighbour, parastichy pair, rise, rung, transitions
  • The response with a hole in it — both name counting blind, divergence angle, ladder, measurement, parastichy pair, rise, rung, transitions
  • The second comb — both name counting blind, divergence angle, lattice, measurement, nearest neighbour, parastichy, parastichy pair, rise

Named objects

A flat tag is an object no other essay names yet.

Counting blindContact networkDivergence angleGeometric ladderHandoverLadderLatticeMeasurementNearest neighbourParastichyParastichy pairRiseRungTransitions