The pattern itself

The symmetry that is not there

A wrecked stem counted 2/6 and a stem grown two organs at a time counted 2/6 are indistinguishable to a spiral counter. Rotate them by half a turn and one lands on itself and the other lands nowhere. A cut does not make a whorled pattern; it makes a pattern that counts like one.

Worth reading first: Counting the spirals · A head is a set of points · Two at a time.

Three of the six places a many-organ cut can send a stem are counted at a pair whose numbers share a factor: 2/6, 4/6 and 3/6. A shared factor is the signature of a whorled pattern — one that arrives k organs at a time and therefore carries k copies of every family — and if a cut could produce one, then the property counting is least able to decide would be reachable by damage.

The test takes one measurement, and it is not a count.

Two patterns a counter cannot tell apart — counted 2/6 against 2/6On the left, the top 90 organs of a spiral stem that never repaired after two organs were removed, settling at 175.01 degrees. On the right, a stem grown by a rule that places two organs at a time on every node. A counter shown the positions returns 2/6 for the first and 2/6 for the second, and a pair whose numbers share a factor is the usual signature of a whorled pattern. Rotate each pattern and the answer separates them at once: the whorled stem maps onto itself at a half turn and the wrecked stem maps onto itself at no fraction of a turn at all. Its shared factor is a fact about where its divergence landed, 4.99 degrees from 1 of 2 turns, and not about how it grew.a wrecked spiral stemthe whorled rule, two at a timesettled at 175.01°three per filecounted 2/6counted 2/6rotational symmetry: order 1rotational symmetry: order 290 organs · cut 3,5 · rise 0.013generated from a stated rule, not drawn to look right
Fig. 1 The whole argument in one frame. A wrecked spiral stem on the left and a stem grown two organs at a time on the right, with what a counter says under each and what a rotation says under that.

Jugacy is a property of the positions

Multijugacy is not a fact about numbers; it is a fact about where the organs are. A pattern is k-jugate when rotating the whole of it by a k-th of a turn maps it onto itself — every organ landing on another organ, to within a small fraction of the local spacing.

three stems: 1, 2, 3 primordia at a time1-jugate at 137.51° counts 2 and 3; 2-jugate at 68.75° counts 2 and 4; 3-jugate at 45.84° counts 3 and 6. Every count shares the factor k, and dividing it out leaves an ordinary lattice: what a k-jugate stem is, exactly, is k copies of an ordinary one wrapped k times round.1 at a time2 and 3symmetry order 12 at a time2 and 4symmetry order 23 at a time3 and 6symmetry order 3divergences 137.51° · 68.75° · 45.84°counted 2/3 · 2/4 · 3/6
Fig. 2 Stems grown at one, two and three organs per node. The symmetry is visible and the counts scale with it, which is why the two are usually treated as the same statement.

That is a different statement from anything a spiral count makes, and this collection has drawn the difference before, on patterns written down from formulas rather than grown: a bijugate lattice and an ordinary lattice at a divergence near half a turn are counted identically and have different symmetry.

Same counts, different patternsBoth are counted 2 and 4 by machinery shown only their positions. Rotating the left one by half a turn maps it onto itself and rotating the right one does not, so the left is bijugate and the right is not — and no count could have said so.two at a time68.75°, bijugatecounted 2 and 4half a turn maps it onto itselfone at a time180.5°, ordinarycounted 2 and 4half a turn does notboth counted 2/4symmetry order 2 against 1
Fig. 3 The distinction demonstrated on two ideal lattices: identical counts, one with a half-turn symmetry and one without.

The measurement is direct. Take the positions, take the median nearest-neighbour distance as the scale, rotate the whole set by 1/k of a turn for every k from two to eight, and ask whether every rotated organ lands within a fraction of that scale of an organ that is already there. The largest k that passes is the order.

Tracing one family: 10 chainsEvery node is joined to the node one repeated displacement away, and the chains that result are drawn separately. There are 10 of them, which is the parastichy number of this family. No index of arrival was used anywhere, which is what lets the same count be made on a pattern where 2 primordia appear at once.10 chains · counted pair 6 and 102-jugate at 69.35° · rise 0.01310 chains in this family
Fig. 4 For contrast, what a counter does with the same positions: follows chains of near neighbours and reports how many chains there are. It never asks what happens under a rotation.

The controls, first

A measurement that never returns anything but one is not a measurement, so the instrument is run on two patterns whose answers are known before it is run on the three in question.

The positive control is a stem the whorled rule actually grew. It is important that it was grown rather than written down: the rule places each organ of a whorl at the minimum of the same profile the ordinary rule uses, with its whorl-mates already in the neighbourhood, so the k-fold symmetry that comes out is a result and not an imposition. A control whose symmetry was built in could not fail.

A bijugate stem answers in pairs, once the half turn is taken outRemoving one organ from a stem grown by a rule that places two at a time, at a rise of 0.013, where the pattern counts 4 and 6 and has rotational symmetry of order 2. The open circles are the displacement of the next organ as it comes out of the arithmetic, which reaches 180° at offsets where the stem has demonstrably not been disturbed — the two organs of a whorl are interchangeable, so calling the other one "next" is a relabelling and not a movement. The filled circles are the same numbers read modulo 180°, which is the only way a 2-jugate divergence is defined. Read that way the response is a run of equal pairs — 71.2°, 71.3°, 34.2°, 34.2° — ending at 6, the larger parastichy number, with everything past it under 1.2°. Two organs of one whorl give the same answer to the last digit, which is the pattern's symmetry showing up in an experiment.45°90°135°180°front 6123456789organ removed, places back from the tipas it comes outmodulo 180°2 organs a whorl · rise 0.013 · counted 4/6 · symmetry 2generated from a stated rule, not drawn to look right
Fig. 5 The whorled rule at work rather than assumed: each organ of a whorl placed against what is already there, with the symmetry left to emerge.

Grown at two organs per node, at the same rise the cuts are made at, it comes out counted 2/6 with rotational symmetry of order 2. Grown at three, it comes out counted 6/9 with order 3. The instrument sees what is there.

Two patterns a counter cannot tell apart — counted 3/6 against 6/9On the left, the top 96 organs of a spiral stem that never repaired after four organs were removed, settling at 235.00 degrees. On the right, a stem grown by a rule that places three organs at a time on every node. A counter shown the positions returns 3/6 for the first and 6/9 for the second, and a pair whose numbers share a factor is the usual signature of a whorled pattern. Rotate each pattern and the answer separates them at once: the whorled stem maps onto itself at a third turn and the wrecked stem maps onto itself at no fraction of a turn at all. Its shared factor is a fact about where its divergence landed, 5.00 degrees from 2 of 3 turns, and not about how it grew.a wrecked spiral stemthe whorled rule, three at a timesettled at 235.00°three per filecounted 3/6counted 6/9rotational symmetry: order 1rotational symmetry: order 396 organs · cut 5,7,9,10 · rise 0.013generated from a stated rule, not drawn to look right
Fig. 6 The three-at-a-time control on the right, counted 6/9 with a third-turn symmetry, beside the wrecked stem counted 3/6.

The negative control is the undisturbed stem the cuts are made in. It is counted 5/8 and its rotational symmetry is order 1 — no rotation maps it onto itself, which is what one organ per height means.

A stem unrolled: 180 nodes at 136.78° with a rise of 0.013 circumferencesThe counter is shown these coordinates and the circumference, and finds 5 parastichies one way and 8 the other. The faint strips left and right are the same stem: a family leaving one edge re-enters at the other.5 and 8rise 0.013 · divergence 136.78°counted 5 and 8, opposed
Fig. 7 The negative control, unrolled. One organ per height, so a rotation by any fraction of a turn has nothing to land on.

How the measurement is made

Worth setting out in full, because a null result stands or falls on whether the instrument could have reported anything else.

The pattern is the top two hundred and twenty organs of a run, taken as points on an unrolled cylinder of circumference one. The scale is the median nearest-neighbour distance, computed from the pattern itself rather than stated, so that a coarse arrangement and a fine one are judged on the same terms.

The same stem, not unrolled90 of the 180 nodes face the reader and 90 are behind the stem, drawn open. The count is 5 and 8 either way; the unrolling changes nothing but the visibility.near facefar face180 nodes at 136.78°5 and 8, both faces
Fig. 8 The object the measurement is made on: positions, and nothing else. No angle, no history, no record of what was removed.

For each order from two to eight, every point is rotated by that fraction of a turn and asked whether an existing point sits within a small fraction of the scale of where it landed. The largest order at which every point succeeds is the answer.

Two details are load-bearing and both were settled when the whorled rule was written, against patterns whose symmetry was known.

The test is made on the interior of the pattern. The top and bottom rows of a finite point set have nothing to rotate onto, so a test applied to all of it reports order one for everything — including a genuinely bijugate stem — and is a measurement that cannot fail.

three stems: 1, 2, 3 primordia at a time1-jugate at 137.51° counts 2 and 3; 2-jugate at 68.75° counts 2 and 4; 3-jugate at 45.84° counts 3 and 6. Every count shares the factor k, and dividing it out leaves an ordinary lattice: what a k-jugate stem is, exactly, is k copies of an ordinary one wrapped k times round.1 at a time2 and 3symmetry order 12 at a time2 and 4symmetry order 23 at a time3 and 6symmetry order 3divergences 137.51° · 68.75° · 45.84°counted 2/3 · 2/4 · 3/6
Fig. 9 The edge in question. At the ends of any finite pattern a rotation has no partner, whatever the pattern’s symmetry is.

And the lookup that finds the nearest existing point lives on the cylinder rather than on a rectangle. A grid keyed on the raw azimuth puts a point at 0.998 of a turn and one at 0.002 in buckets a whole turn apart, so every query near the seam misses — and nine per cent of a spiral pattern lies within a cell of the seam, which is exactly where its neighbours are. That bug once reported a bijugate lattice with eight parastichies in a family as having thirty-one.

Six stems built, forgotten and recoveredEach row is a lattice built from a divergence and a rise, counted by machinery shown only the coordinates, and reconstructed from the counts and the two hop lengths. The worst error in the recovered angle is 3.0e-13°.137.51°, rise 0.092.8e-14°counted 2/3137.51°, rise 0.032.0e-13°counted 3/5137.51°, rise 0.0122.8e-14°counted 5/899.50°, rise 0.083.0e-13°counted 1/3151.14°, rise 0.071.4e-13°counted 2/399.50°, rise 0.021.1e-13°counted 4/7error in the recovered divergence anglecounts and hop lengths onlyworst 3.0e-13°
Fig. 10 The surface the lookup has to live on, and the reason: a stem has a seam, and the neighbours of a point near it are on the other side of it.

The three destinations have order one

All three.

destination counted shared factor rotational symmetry
175.01° 2/6 2 1
189.96° 4/6 2 1
235.00° 3/6 3 1
Two patterns a counter cannot tell apart — counted 4/6 against 2/6On the left, the top 90 organs of a spiral stem that never repaired after four organs were removed, settling at 189.96 degrees. On the right, a stem grown by a rule that places two organs at a time on every node. A counter shown the positions returns 4/6 for the first and 2/6 for the second, and a pair whose numbers share a factor is the usual signature of a whorled pattern. Rotate each pattern and the answer separates them at once: the whorled stem maps onto itself at a half turn and the wrecked stem maps onto itself at no fraction of a turn at all. Its shared factor is a fact about where its divergence landed, 9.96 degrees from 1 of 2 turns, and not about how it grew.a wrecked spiral stemthe whorled rule, two at a timesettled at 189.96°three per filecounted 4/6counted 2/6rotational symmetry: order 1rotational symmetry: order 290 organs · cut 5,6,8,9 · rise 0.013generated from a stated rule, not drawn to look right
Fig. 11 The second of the three, at 189.96 degrees and counted 4/6, beside the same bijugate control. The counts share a factor of two and only one of the panels has a half-turn symmetry.

The strongest form of the comparison pairs them off rather than reporting the number alone. The stem that settles at 175.01° is counted 2/6. The stem the whorled rule grew at two organs per node is counted 2/6. A counter shown the positions of both returns the same pair and has nothing further to say. Rotated by half a turn, the second maps onto itself and the first does not — not marginally, not at a looser tolerance, not at any order from two to eight.

The round trip, for every jugacyEach pattern is built from a divergence, the divergence is thrown away, the families are counted by tracing chains, the jugacy is read off the symmetry, and the divergence is recovered. The worst error over the four is 1.1e-13 degrees — and each answer is modulo the pattern's own period, 360/k, because adding that leaves the point set identical.jugacycountedperiodaskedrecoverederrork = 12 and 3360.0°138.4078°138.4078°1e-13k = 24 and 6180.0°69.6539°69.6539°1e-13k = 36 and 9120.0°46.7359°46.7359°0e+0k = 48 and 1290.0°35.2769°35.2769°3e-14160 whorls each · counted by tracing chainsworst error 1.1e-13°
Fig. 12 The counter checked against a whorled pattern it is shown deliberately: the pair is recovered and so is the divergence, so the instrument is not failing to see jugacy when jugacy is there.

So a cut does not convert a spiral stem into a whorled one. The rule kept placing one organ at a time throughout, which is what it always does, and the pattern it produced is a one-organ-at-a-time spiral whose two shortest families happen to share a factor.

The rule, 26 steps in, at a growth of 0.40The next primordium goes where the repulsion is least — the marked minimum at 216°. Nothing in the rule refers to any particular angle.05e+51e+61.5e+60100200300angle around the boundary (°)repulsion from what is theregrowth 0.40 · 14 elements in playthe minimum is where the next one goes
Fig. 13 The reason that is the expected answer rather than a surprising one: nothing in the placement changes when organs are removed. One organ, one height, one minimum.

The inference that fails, stated as an inference

It is worth writing out the step that breaks, because it is a step almost nobody writes down and almost everybody takes.

A pattern with k organs per node has k-fold rotational symmetry. True, by construction.

A pattern with k-fold rotational symmetry has every parastichy family in k copies. True: the rotation carries each family to another family of the same count.

Therefore a pattern whose counted pair shares a factor of k has k organs per node. False. It reverses an implication. Sharing a factor is a consequence of the symmetry and is not equivalent to it, and the three destinations here are exactly the counterexample.

The 3-jugate forks converge on 45.8359°Every fork sits at a rational divergence, with denominator 6(m² + mn + n²) — 15/42, 45/114, 111/294 and so on. The limit is 45.8359°, which is 137.5078 divided by 3, and it is at none of them.44461234fork number down the treedivergence at the fork (°)3/66/99/1515/24137.5078/3 = 45.8359°3-jugate · 4 forkslast fork 46.0465°
Fig. 14 The arithmetic the true half of the inference lives in: a k-jugate pattern’s pairs are an ordinary pattern’s pairs multiplied through, all the way down.
The Fibonacci share, read two waysAt a rise of 0.006 only 11.4 per cent of divergences give a pair of consecutive Fibonacci numbers. Allow a common factor to be divided out first and it is 49.8 per cent. The whole of the increase is pairs of the form k and 2k — k copies of the bottom rung — which is a generous reading that describes no plant.rise 0.026, strictly29.7%rise 0.026, up to jugacy56.2%rise 0.006, strictly11.4%rise 0.006, up to jugacy49.8%share of divergences2 rises · 220 divergences each11.4% → 49.8% at rise 0.006
Fig. 15 And the census that shows the converse has room to fail in: which pairs appear at which divergences and which jugacies, with shared factors reachable from more than one direction.

The reason the reversal usually works is empirical rather than logical. Ordinary spiral patterns sit near the golden angle, where no small number of consecutive steps comes back near the start, so an ordinary pattern’s shortest two families are consecutive Fibonacci or Lucas numbers and are coprime. A pair with a factor in it therefore usually does mean a whorl — because the other way of getting one requires a divergence nothing normally arrives at.

What a divergence picked at random gives, at a rise of 0.026Fibonacci pairs take 29.7% of the circle at this rise, and the share falls as the rise does. The claim that Fibonacci counts are what nature "prefers" needs the preference to come from somewhere, and it is not from the geometry being generous.Fibonacci29.7%Lucas5.1%whorled26.4%other38.9%15 distinct pairs over 1200 divergencesrise 0.026Fibonacci 29.7%
Fig. 16 The empirical fact the reversal rests on: swept across the rises, the pairs an ordinary stem gives are coprime everywhere.

A cut is a way of arriving at one.

Why the counter is not wrong

It is worth being careful here, because “the counter says 2/6 and the pattern is not bijugate” reads like an instrument failure and is not one.

The counter’s job is to report the two families of nearest chains in the positions. At a divergence of 175.01° that is exactly what it does: consecutive organs sit almost opposite each other, so the pattern really does have two near-vertical rows of organs and really does have six chains in the other direction. Two and six are the right answer to the question the counter is answering.

Two patterns a counter cannot tell apart — counted 2/6 against 2/6On the left, the top 140 organs of a spiral stem that never repaired after two organs were removed, settling at 175.01 degrees. On the right, a stem grown by a rule that places two organs at a time on every node. A counter shown the positions returns 2/6 for the first and 2/6 for the second, and a pair whose numbers share a factor is the usual signature of a whorled pattern. Rotate each pattern and the answer separates them at once: the whorled stem maps onto itself at a half turn and the wrecked stem maps onto itself at no fraction of a turn at all. Its shared factor is a fact about where its divergence landed, 4.99 degrees from 1 of 2 turns, and not about how it grew.a wrecked spiral stemthe whorled rule, two at a timesettled at 175.01°three per filecounted 2/6counted 2/6rotational symmetry: order 1rotational symmetry: order 2140 organs · cut 3,5 · rise 0.013generated from a stated rule, not drawn to look right
Fig. 17 More of the same stem, so the two files are visible as files. The counter is reporting them, and they are there.

What is wrong is the inference. “A pair with a shared factor implies k organs per node” is a rule of thumb that holds across the patterns botanists usually meet, because those patterns sit near the golden angle where no small number of consecutive steps comes back to the start. It fails for a lattice that has drifted somewhere else, and a wrecked stem has drifted somewhere else by construction.

The spiral counts four different divergence angles produceFibonacci counts come from one angle. The Lucas angle — which the same dynamical model reaches on a different branch — gives 47 and 76, and neither number is a Fibonacci number.golden 137.51°55 and 89FibonacciLucas 99.50°47 and 76Lucas151.14°50 and 81neither77.96°37 and 60neithercounted from the pointsone sequence per branch
Fig. 18 Where the rule of thumb comes from and where it stops: the pair a counter returns as the divergence is swept, with the shared factors appearing at particular angles rather than everywhere.
How nearly each angle is a simple fraction of a turnA dip means a rational approximation and a lattice with visible rows. The golden angle's floor is 0.008; the rational angle reaches exactly zero.00.2000.400204060denominator qhow nearly q × angle is a whole turn (0 = exactly)golden 137.508°137.3°135° = 3/8distance to the nearest whole turnno dips means no rows
Fig. 19 And why those angles are where they are: the fractions with small denominators are the places a few consecutive steps nearly close, and they are sparse.

What would have had to be true

Suppose the answer had gone the other way. It is worth being explicit about what that would have meant, because a test whose alternative outcome has no consequences is a test nobody needed to run.

A rotation of half a turn mapping a wrecked stem onto itself would mean that organ i and some organ at nearly the same height sit nearly opposite each other, for every organ in the run. The rule places one organ per height, so the partner would have to be an organ at a different height that happened to land there — and it would have to happen for all two hundred and twenty of them at once, to within a fraction of the local spacing.

A stem unrolled: 180 nodes at 175.00° with a rise of 0.013 circumferencesThe counter is shown these coordinates and the circumference, and finds 2 parastichies one way and 4 the other. The faint strips left and right are the same stem: a family leaving one edge re-enters at the other.2 and 4rise 0.013 · divergence 175.00°counted 2 and 4
Fig. 20 What would have to line up: every organ paired with another at a half turn’s remove and nearly the same height, throughout the run.

There is a rise at which that is nearly true, and it is worth naming because it is the case that makes the test non-trivial. If the rise were small enough that consecutive organs were separated vertically by much less than the local spacing, a stem near half a turn would approach a two-ranked arrangement in which organs really do pair off. The rises here are not small enough — at 0.013 the vertical step is more than a tenth of the spacing — but the failure is quantitative rather than categorical, and a test with a tolerance stated relative to the spacing is what turns that into a number.

A whorl and a spiral, from one lattice at two divergencesAt 180° the nodes fall on 2 rows and the two counts share a factor: the elements of each turn are level with one another. At 137.51° they never are.180° — a half turn2 and 4 — whorled137.51°3 and 5 — Fibonaccirise 0.020 in both panelsthe counts decide, not the eye
Fig. 21 The arrangement the wrecked stem would have to be approaching, at a rise where organs really do pair off.
Same counts, different patternsBoth are counted 2 and 4 by machinery shown only their positions. Rotating the left one by half a turn maps it onto itself and rotating the right one does not, so the left is bijugate and the right is not — and no count could have said so.two at a time68.75°, bijugatecounted 2 and 4half a turn maps it onto itselfone at a time179.4°, ordinarycounted 2 and 4half a turn does notboth counted 2/4symmetry order 2 against 1
Fig. 22 And the pair of patterns the whole distinction rests on, drawn closer to the case that matters: a genuinely bijugate lattice and an ordinary one near half a turn.

So the null is not “the measurement found nothing”; it is “the measurement found order one where a stated alternative would have given two, on a pattern the alternative’s own signature was extracted from”.

What a wrecked stem is doing instead

Two things are worth saying about the object itself, because “not whorled” is a negative and the positive description is short.

The first is that it is a lattice. The three destinations are settled: the divergence holds to a fraction of a degree over the last hundred and twenty organs, the counter returns a stable pair, and the positions form a proper two-family packing. Nothing here is a stem in the middle of falling apart.

The block a wrecked stem settles into is the count it was cut fromA stem is cut in the middle of its front and followed for 300 organs. It does not come back to its lattice; what it does instead is repeat a fixed sequence of divergences exactly, to the resolution of the azimuth grid. Each row shows that sequence twice over, one bar per organ, drawn to the same scale. At the 5/8 rung the sequence is five angles long and advances -36.1° per block. Every block is the smaller number of the pair that was cut, so the second attractor carries the first one's count — and every precession is one part in twice the block, which makes each of these a two-jugate arrangement with 10 rows.5/8 rungblock of 5-36.1° a blockand again208.8° on average300 organs after the cut · 1536 azimuthsgenerated from a stated rule, not drawn to look right
Fig. 23 The evidence that a destination is a destination: after the transient, a fixed sequence of divergence angles repeating without end rather than a wander.
The angles against the positions, rise by risetwo rises, five seeded stems each. A filled mark is a run whose angle readout returned the pair the position counter finds in the same stem; an open mark is a refusal. At 0.013 the counter says 5/8 and the angles agree on 5 of 5. At 0.005 the counter says 8/13 and the angles agree on 5 of 5. The two instruments share no code path: one is given a list of angles, the other a list of coordinates.risefive stems, read from the angles alonethe position counter0.0135/85/85/85/85/85 and 80.0058/138/138/138/138/138 and 13seeded at 137.3°, 900 nodes per stemfilled where the two instruments agree
Fig. 24 The pair extracted from the angles alone, as a cross-check on the pair extracted from the positions. Two instruments, and they agree on undisturbed stems.

The second is that it is a lattice the rule can occupy and never reaches on its own. Grown from a golden seed at this rise, the rule settles at 136.78° every time; grown from a Lucas seed it settles somewhere else; and nothing in the undisturbed sweep of this collection has ever produced 175.01°. It is a state the placement rule is perfectly happy to sit in and has no route into, except by having something taken out of it.

Placements that went to a different minimum, per thousandThe rule's own counterfactual, run beside it: where would this node have gone with the noise taken away and everything else left alone? Placement noise displaces the node after the argmin, so the answer is always "here" — 0.2°, 0.4°, 0.8° all give zero. A jostle and a field perturbation are upstream of the choice and change one or two placements in a thousand while the lattice is still intact.field 0.0052.10.70° of scatterfield 0.00750.01.00° of scatterfield 0.010.01.12° of scatterjostle 0.22.10.89° of scatterjostle 0.41.10.87° of scatterjostle 0.81.11.12° of scatterplacement 0.20.00.78° of scatterplacement 0.40.00.94° of scatterplacement 0.80.01.42° of scatter3 runs each · a basin change is half a local spacingplacement noise: zero by construction
Fig. 25 The general shape of that: which state the rule settles into depends on where it starts and what it is disturbed by, and the reachable states are not all the stable ones.
four limit divergences, all of them 137.5078 over a whole numberThe 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.1-jugate137.5078°counts 3/52-jugate68.7539°counts 6/103-jugate45.8359°counts 9/154-jugate34.3769°counts 12/20limit divergence4 jugacies137.5078 / k
Fig. 26 And the states the rule can hold at all, laid out. The destinations of a cut are among them; the ones it arrives at unaided are a much smaller set.

What this closes and what it opens

It closes the alarming reading. Jugacy is not reachable by damage in this rule, and a specimen counted with a shared factor is not evidence that something was removed from it. The measurement that decides is available on any pattern whose positions can be recorded, and it is one rotation.

The Fibonacci share, read two waysAt a rise of 0.008 only 14.6 per cent of divergences give a pair of consecutive Fibonacci numbers. Allow a common factor to be divided out first and it is 49.7 per cent. The whole of the increase is pairs of the form k and 2k — k copies of the bottom rung — which is a generous reading that describes no plant.rise 0.03, strictly31.2%rise 0.03, up to jugacy55.8%rise 0.008, strictly14.6%rise 0.008, up to jugacy49.7%share of divergences2 rises · 200 divergences each14.6% → 49.7% at rise 0.008
Fig. 27 The census the closure is set against: which jugacies the whorled rule produces at which rises, none of which the ordinary rule reaches at any divergence.

It opens a smaller and more tractable question. If the shared factor is a fact about where the divergence landed rather than about how the organs arrived, then the three destinations should have something in common that the other three do not — some property of 175.01°, 189.96° and 235.00° that 136.99°, 208.80° and 280.43° lack.

Everywhere a cut of one to five organs can send a 5/8 stemEvery settled divergence reached by any arrangement of up to five organs removed from a stem at the 5/8 rung, on one axis. There are six of them and no more. three are slips of the lattice the stem was cut from: each keeps the lag-5 family intact and sits a whole number of turns of it from the next, which is the ladder marked below the axis with rungs 72.0 degrees apart. The other three keep no lag at all and sit near a fraction of a turn, marked above: 175.0 degrees near 1 of 2 turns, 190.0 degrees near 1 of 2 turns, 235.0 degrees near 2 of 3 turns. A stem that is cut either slides along the ladder it was on or leaves it for a lattice with files in it.120°150°180°210°240°270°300°1/2 of a turn2/3 of a turn175.0°counted 2/6190.0°counted 4/6235.0°counted 3/6137.0°0 turns208.8°1 turn280.4°2 turnssettled divergencethe ladder: one turn of the lag-5 family is 72.0°cuts of one to five organs at a rise of 0.013 · 6 destinationsgenerated from a stated rule, not drawn to look right
Fig. 28 The six destinations again, with the three that count with a factor marked above the axis and the three that do not marked below.

They do, it is measurable in one line, and getting the measurement right turns out to matter more than it looks — because the obvious version of it reports that the golden angle has five files, which is the exact opposite of the fact the whole subject rests on.

Shares its objects with

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

  • A survivor has to be a neighbour — both name ablation, counting blind, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • Half a turn, four at a time — both name ablation, counting blind, classification, honest limits, lattice, measurement, negative result, parastichy pair
  • One offset, two answers — both name ablation, control, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • Three organs and no mirror — both name ablation, counting blind, control, falsifiability, honest limits, lattice, measurement, parastichy pair
  • Two accounts of one number — both name ablation, counting blind, honest limits, jugacy, lattice, measurement, negative result, parastichy pair
  • A period that is not a count — both name ablation, counting blind, falsifiability, honest limits, lattice, measurement, parastichy pair

Named objects

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

AblationBijugateCounting blindClassificationControlFalsifiabilityHonest limitsIdentifiabilityJugacyLatticeMeasurementNegative resultParastichy pairRotational symmetryWhorled