Where the angle comes from

One rung, two answers

The offset accounts for twenty-five wrecked stems of thirty and is refuted by a single pair of runs that differ in nothing but the rise. Sweep one rung at a thousandth and the refutation stops being an anomaly: the same offset on the same lattice keeps one family at the coarse end and the other at the fine one.

Worth reading first: The organ that was taken away · Counting the spirals · A head is a set of points.

A stem that never repairs after organs are removed keeps one lattice hop rigid, and the hop it keeps is one of the two contact families at twenty-nine of thirty offsets. Which of the two is not decided by which is shorter. The best account left standing is the offset — take the smaller counted number if the removal landed no further back than it, the larger if it landed beyond — and it is right at twenty-five of thirty.

It is refuted by exactly one thing, and the refutation is worth restating precisely because it is so small. Two runs agree on the counted pair, agree on the offset, and disagree on which family survives. They differ in the rise.

Which family survives, along the 5/8 rung. The family a wrecked stem keeps, at every offset that wrecks and every rise on one rung. A counter shown any of these stems returns 5 and 8 spirals, at all twelve rises, so nothing in the pair distinguishes the columns. The cells say otherwise: at an offset of 4 the stem keeps the 5-family at the coarse end of the rung and the other one at the fine end. The offsets that wreck at all grow from 1 to 5 as the rise falls, because the front deepens, and the extra offsets are the ones that keep the larger number. So the rule stated over the offset alone is a rule with the rise left out of it.
Fig. 1 The whole of this essay in one picture. Offset down the side, rise across the top, and the family left standing written in the cell.

A single disagreeing pair is the kind of result that can be a mistake, a tolerance, or a seed. This essay makes it reproducible by sweeping the quantity the two runs differed in — and it turns out not to be an anomaly at all but the ordinary behaviour of a rung, invisible until now because every census this collection has run sampled one rise per rung.

A rung, swept at a thousandth

A rung is a range of rises over which a counter returns the same pair. Sampling one rise from each is the natural thing to do when the question is which pair, and exactly the wrong thing when the question is what else varies.

Swept from 0.018 down to 0.007 in steps of a thousandth, twelve rises return the same pair. Nothing a counter can measure separates them.

The choice of a thousandth is not arbitrary and it is the only free parameter in the sweep, so it is worth stating what it buys. Coarser than that and the rung holds four or five samples, which is what every earlier census here effectively used and is too few to see an ordering reverse inside it. Finer and each stem still settles, but the twelve rises become twenty-four that say the same thing at twice the cost, because what is being resolved is a monotone slide rather than a feature with a width. A thousandth is the resolution at which the rung stops being a point and has not yet become a continuum.

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. 2 What a rung is, and how much geometry it hides. Sweeping the rise, the counted pair holds constant over a range and then steps.
How many offsets wreck, along the 5/8 rung. The count of offsets that never repair, at each rise on one rung. It runs from 1 at the coarse end to 5 at the fine end, while a counter returns 5 and 8 spirals at every one of them. The front — the run of recent organs at which a removal is felt at all — deepens as the rise falls, so there are simply more places a cut can land and fail to heal. That is the mechanism under the grid: the offsets that appear at the fine end are the ones beyond the smaller contact number, and those are the ones that keep the larger family.
Fig. 3 The first thing that moves: how many offsets never repair, at each rise of the rung.

Two quantities move across those twelve rises, and a counter is blind to both.

That blindness is not a defect of the instrument. A spiral count is deliberately a topological reading: it follows chains of near neighbours and reports how many run in each direction, and it returns the same answer for every arrangement in which those chains connect the same way. A whole rung is, by construction, the set of geometries about which it says one thing. So asking a counter to distinguish two stems inside a rung is asking it to do the opposite of its job, and any account of ablation stated purely in counted numbers inherits that limit whether or not it declares it.

The divergence slides, and the two steps change places

The settled divergence runs from 136.5469° at the coarse end to 137.8672° at the fine one — a slide of one and a third degrees, monotonic apart from a flat pair at the top, and entirely inside one rung.

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. 4 The settled divergence at each rise of the rung. A counter shown any of these stems reports the same thing about all of them.

The second is sharper, and it is the one this collection has an argument riding on. Rank the lags by the length of their step across the surface — the distance the placement rule itself uses — and the two contact families come first and second. Which of them is first changes hands inside the rung.

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. 5 The ratio of the second step to the shortest. It falls to within one and a third per cent at a rise of 0.016 and the ordering reverses at 0.015.

At the coarse end the shorter step belongs to the smaller family. At 0.016 the two are within 1.3 per cent of each other. From 0.015 down the shorter step belongs to the larger family. The whole reading that “the rule keeps its shortest hop” was refuted against is a statement about an ordering that reverses under a parameter the counter cannot read.

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. 6 The ranking at the coarse end of the rung, where the smaller family carries the shorter step.
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. 7 And near the fine end, where the same lattice by every count a counter makes has the ordering the other way round.

The survivor changes hands with it

The offsets that never repair grow from one at the coarse end to five near the fine one. That is the front deepening: the run of recent organs at which a removal is felt at all is the larger of the two counted numbers, and as the rise falls there are simply more places a cut can land and fail to heal.

The next organ moves for the last 8, and for no others. One row per organ removed, counted back from the tip of a stem at a rise of 0.013 whose counted pair is 5 and 8. Removing any of the last 8 moves the next organ by 4.9° to 164.1°; removing an older one moves it by at most 0.70°, which is under the azimuth grid. The boundary is at 8, and 8 is the larger parastichy number — so the experiment counts the spirals without measuring an angle.
Fig. 8 Why the offset is a quantity the answer can depend on: the immediate effect of a removal varies enormously with where it lands.
On a rung the response is a run of offsets; near a transition it has a hole. One row per rise, from 0.032 at the top to 0.005 at the bottom, and one column per offset: the organ one place back at the left, 14 places back at the right. A cell is filled where removing that organ moves the next organ by more than 2.5°, and empty where it does not. On a rung the filled cells are a run from one to the larger parastichy number — 5, 8, 13 at the pairs shown on the left. Every rise shown here is in the middle of its rung, so every row is a run and nothing past it is felt — what happens between the rungs is a separate matter.
Fig. 9 And the range it varies over, which is what sets how many offsets can wreck at all.

The deepening is worth separating from the survivor question, because it is the part that needs no new mechanism. A front three organs deep offers three places to cut; a front eight organs deep offers eight. If the rule for which family survives were written down correctly and never changed, the number of wrecked offsets would still grow down a rung simply because there are more offsets. What the grid adds is that the offsets which appear at the fine end are not a random extension of the ones already there: they are the offsets past the smaller counted number, and they are exactly the ones that keep the larger family.

Read the grid along any row and the counted pair is constant. Read down the row at an offset of four:

  • from 0.018 to 0.008 it keeps the five;
  • at 0.007 it keeps the eight.
Which family survives, along the 5/8 rung. The family a wrecked stem keeps, at every offset that wrecks and every rise on one rung. A counter shown any of these stems returns 5 and 8 spirals, at all twelve rises, so nothing in the pair distinguishes the columns. The cells say otherwise: at an offset of 4 the stem keeps the 5-family at the coarse end of the rung and the other one at the fine end. The offsets that wreck at all grow from 1 to 5 as the rise falls, because the front deepens, and the extra offsets are the ones that keep the larger number. So the rule stated over the offset alone is a rule with the rise left out of it.
Fig. 10 The same grid without the marking, so the columns can be read as a sweep rather than as a claim.

Same lattice. Same pair. Same offset. Different survivor. The disagreement that appeared once in the census appears here on demand, and the thing that produces it is the position on the rung.

Take away the organ four places back, and the next one goes into the hole. The last 30 organs of a stem at a rise of 0.013, unrolled. The open circle is the organ removed — four places before the tip. The ring at the top is where the rule puts the next organ with every organ present; the filled mark beside it is where the rule puts it with that one missing. The two are 164.1° apart, against a local spacing of 41°, and the vacancy itself is 172.7° from the undisturbed answer. Nothing else differs between the two runs: same rise, same history, same rule.
Fig. 11 The intervention, held fixed: one organ removed four places back, with the rise the only thing that varies between the columns of the grid.
One wrecked stem, lag by lag — golden, rise 0.013, organ 4 back. How much each lattice hop moves from organ to organ in a stem that never repaired after a single removal, over its last 120 organs. The lag-one hop is the divergence itself and it swings by 65 degrees. The lag-5 hop swings by 0.11 degrees and sits 0.09 degrees from where the undisturbed stem put it, so that one family of the original lattice is still standing organ by organ. Its multiples inherit the same steadiness and nothing else comes within a factor of twenty. The block of angles this stem repeats has a period of 5, which is the surviving lag and not a coincidence.
Fig. 12 One of these stems read by lags rather than by neighbours, which is the measurement the surviving family is defined by.

What this does to the rule

The offset rule is not overturned by this. It is relocated.

Its first clause — a cut inside the smaller count leaves the smaller family standing — holds at every offset it applies to, at every rise of the rung, with one exception at the very fine end. Its second clause is the one that needs a rise attached: the offsets beyond the smaller count only exist once the front is deep enough to have them, and they are the ones that keep the larger family.

It is worth putting a number on how much of the rung each answer owns, because the number is uncomfortable.

Offset four is the offset the two disagreeing runs shared. Across the twelve rises of this rung it keeps the five at eleven of them and the eight at one; the crossing sits at the fine end, between 0.008 and 0.007, and only a single rise inside the rung lies below it. The column is not evenly divided. It is eleven to one.

That ratio is this essay’s own result read backwards, and it says something awkward about how the result was found. A census that samples one rise per rung draws one cell from that column. Eleven times in twelve it draws a five, agrees with the rule stated over the offset, and records a row that supports it. Once in twelve it draws an eight, disagrees, and records the anomaly that sent this sweep out in the first place.

So the refutation was available only because the sampling was unlucky, and unlucky by about one part in twelve, on one offset, of one rung. The history in which the census happened to sample 0.009 rather than 0.007 is a history in which the offset rule scores twenty-six of thirty rather than twenty-five, nothing looks wrong anywhere, and the missing ingredient stays invisible for exactly as long as nobody sweeps a rung.

The general form of that applies to every row this collection has published from a one-rise census. A rule that is right at eleven of twelve rises and wrong at the twelfth will be scored as right, with a small residue of anomalies, by any procedure that samples one rise per rung. The residue is not noise, and it does not shrink as more stems are measured: it is a fixed fraction of the rung’s width, so measuring more stems one rise at a time estimates that fraction more precisely while doing nothing whatever to explain it.

Which lag survives, at every lattice and every offset. A row for each of twelve lattices and a column for each offset an organ is removed at, with the lag whose hop survived written in the cell. 30 cells never repair. The lag left standing is one of the two contact families at 29 of them, and at 17 it is the second shortest step on the lattice rather than the shortest, which is what refuses the reading that a rule holds its nearest neighbours. The ringed cells are the five the offset rule gets wrong. Two lattices carry no cells at all because no single removal wrecks them.
Fig. 13 The census the rule was scored on, one rise per lattice. Every column of this essay’s grid would have been a single cell here.

So the rule stated over the offset alone is a rule with the rise left out, and quoting it without the rise quotes half the argument. The honest form is conditional: given a front of this depth, the offset decides. The depth is a function of the rise, and the rise is exactly what a counter throws away.

Stated that way the rule stops being a fit and starts being a claim with a domain, which is the difference this collection keeps insisting on. A rule that scores twenty-five of thirty over a census assembled from one rise per rung is being scored on a sample that never varies the thing it depends on. The same rule scored along a rung — where the offset is held and the rise moved — is either right at every rise or it is not, and here it is not.

A second cut moves the next organ, and does not move the boundary. Every pair of organs that can be taken out of a settled stem at a rise of 0.032, where the pattern is 3/5. A row is the offset of the nearer organ removed, counted back from the tip; a column is how many further places back the second one sits. The shade is how far the next organ ends up from where it would have been, from under a degree in the palest cells to a half-turn in the darkest. The run of shaded rows ends at 5, which is the larger parastichy number, and every row below it is blank across the whole width — the largest displacement anywhere past the front is 2.34°. So the nearer of the two organs decides whether the removal is felt at all, and the second one, wherever it is put, cannot make the pattern notice an organ it was not going to notice.
Fig. 14 The shape of the table these offsets come from, at a rung where the front is shallow enough to see the whole of it.
The block is one of the two numbers, and not always the smaller. Every lattice a single organ was removed from, one row each: golden, rise 0.013 carrying 5/8; golden, rise 0.008 carrying 5/8; golden, rise 0.005 carrying 8/13. The two open ticks on each line are that lattice's own parastichy numbers; the filled dots are the blocks the stems that never recovered settled into, one per offset that failed. The claim this table was built to test is that the block is the smaller of the two, which held at the two rises it was first measured at. It does not hold here: 5/8 gives 5 and 8. What survives is weaker and still worth something — every filled dot but 1 sits on one of that row's own ticks, so the orbit carries a count of the lattice it was cut from, and which of the two it carries is decided by the offset rather than by the pattern.
Fig. 15 The same conclusion in the quantity that first raised the question: the period of the motif a wrecked stem repeats, which equals the surviving family.

Three controls

The pair really is constant. The claim is worth nothing if the sweep quietly crosses a rung boundary, so the counted pair is measured at every rise and the generator refuses to draw a grid whose columns are not all the same pair. Twelve of twelve return the same two numbers.

What the finer grid does to the rises already published. The two rises this site has argued from and the one it published as having no answer, each read at both azimuth grids, five stems apiece. A filled mark agrees with the position counter, a half mark contradicts it, an open mark is a refusal. At 0.013 and 0.005 the readings are identical at both grids, so nothing already written depends on the sample count. At 0.008 they are not: 384 azimuths gives 5/8, 5/8 and 1152 gives 8/13, 8/13, against a counter that says 5/8. That rise was chosen in the earlier work because the three shortest lattice offsets there are within a fifth of each other, and a stem with no answer answering differently on a different grid is the object behaving as it was said to.
Fig. 16 The counter, checked against the positions rather than trusted: what a grid of a stated fineness can and cannot resolve.

The steps are not tied. At 0.016 the two contact steps differ by 1.3 per cent, which is small enough to ask whether the ordering there is a measurement rather than a fact. It is a fact about the geometry — the lengths are computed from the settled divergence and the rise, not estimated from a drawing — but the essay does not rest on that rise. The survivor changes hands at 0.008 to 0.007, five rises away from the crossing, where the two steps differ by seven per cent.

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. 17 The families a wrecked stem chooses between at one lattice. The slider walks the census, and the marked bars are what was actually left standing.

And the sweep is not an artefact of its own resolution. A thousandth is fine enough to put twelve rises inside this rung and coarse enough that each is a settled lattice by the same test every other run on this site uses.

A window that fits inside a rung. Stems that climb the ladder at four rates, read over a window at the fine end. The condition is a ratio: the window has to be shorter than a rung. 250 internodes at 260 per rung is 0.96 rungs and agrees on 3 of 3; 400 internodes at 260 per rung is 1.54 rungs and agrees on 1 of 3; 250 internodes at 520 per rung is 0.48 rungs and agrees on 2 of 3; 400 internodes at 520 per rung is 0.77 rungs and agrees on 3 of 3. Read over the whole stem instead, every rate returns nothing — 0 of 3, 0 of 3 — because the quantity the comb is periodic in changes as the pattern climbs.
Fig. 18 The general form of the caution: a window read inside one rung, where the pair is fixed and everything else is not.
Every open question here needs under 28 specimens. The sample size at which each comparison reaches 80 per cent power at a 5 per cent false-positive rate, from the exact binomial rather than a normal approximation. The census question — do plants show consecutive Fibonacci pairs far more often than the geometry does — needs 4: 14.7% is the share of divergence angles giving a consecutive Fibonacci pair at a fine rise; 90% is what a grown history gives.
Fig. 19 And the form the caution takes when the claim is about a real plant rather than a run: how many independent cases a difference of a stated size needs.

What is left over

Two things this does not settle, and both are worth naming rather than implying.

Which of the two moving quantities is the one that acts. The divergence slides and the step ordering reverses across the same rises, so this sweep cannot separate them: any rule written over the position on the rung fits, and so does any rule written over the step ratio. Separating them needs a lattice where the two come apart — a branch on which the divergence slides one way and the ordering the other — and whether such a rung exists is a question about the arithmetic of the ladder rather than about ablation.

The block a wrecked stem settles into is the count it was cut from. A 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; At the 8/13 rung the sequence is eight angles long and advances 22.5° 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 and 16 rows.
Fig. 20 What the disagreement decides, in the end: two wrecked stems settle into motifs of different length, and the length is the family that was kept.
The newest member of the front is the weakest. For every cell of the design whose rung boundary is inside the range, how far the next organ moves when the organ exactly as many places back as the larger parastichy number is removed — the offset that arrived when the stem entered this rung — against how far below that boundary the stem sits. Each line is one lattice on one branch. The horizontal line is the threshold that decides whether an offset counts as felt, and the one cells below it are the one whose front reads one offset short. Nothing is a different kind of thing: the boundary is a step everywhere, and near the top of a rung its last stair is shallow.
Fig. 21 The measured gradient inside a rung: the strength of the response at the newest member of the front, growing steadily as the stem gets finer.

Whether the same thing happens on the other branch. Everything here is one rung of the golden branch. The Lucas branch has rungs of its own and its own ordering of contact steps, and the pair of runs that started this was a Lucas pair.

The same rule, the same rise, two lattices, two fronts. How many organs back a single removal is still felt, on a stem seeded onto the golden lattice and on one seeded onto the Lucas lattice, at seven rises. Everything but the seed is identical at each rise — the rule, the spacing, the heights, the azimuth grid — and the two fronts differ at every one of them. Which branch has the wider front changes hands four times going down the range, so no function of the rise gives the column. The golden branch carries 5/8 at four of these rises, across a factor of two in the rise, and its front is eight at all four.
Fig. 22 The two branches carry fronts of different depth at the same rise, so a rung on one is not a rung on the other.
The band that never heals is what two fixed edges leave over. Each row is one rung. A stem is grown to 400 organs, one organ is removed, and the stem is followed for 300 more. A filled mark is an offset the stem recovers from, with the number of organs it took printed above it; an open ring is an offset it never recovers from. At the 3/5 rung, a front of 5, every offset heals. At the 5/8 rung, a front of 8, the offsets 4, 5 never heal. At the 8/13 rung, a front of 13, the offsets 4, 6, 7, 8, 9 never heal. What is the same at every rung is the two edges: the first three offsets heal, and so do the last few of the front. What is left in the middle is the band, and it widens because the front does.
Fig. 23 And the coarsest version of the same point: whether a stem is wreckable at all is a property of where it sits, not of the pair it is counted at.

Where this leaves the question

The question this thread has been asking since the first removal is what decides which hop the rule keeps, and the answer has been narrowed three times: to one of two families, then to not-the-shorter, then to the offset at twenty-five of thirty. This narrows it a fourth time, and it is the first of the four that adds an ingredient rather than removing one.

Agreement between two windows happens only on a slow enough shoot. Five stems at each of four rates and five disturbances, each read through two overlapping windows of 250 internodes. A filled mark is agreement — both windows reported the same pair; a half mark is a disagreement; a small mark is one window reporting and one refusing; an open mark is silence. Agreement appears 0 times in 25, 1 times in 25, 14 times in 25, 14 times in 25 at 130, 250, 400, 700 nodes per rung, and the two rates it is almost absent from are the two at which a rung is no longer than the window.
Fig. 24 The general shape of a scored comparison: several stated readings, one table, and the score reported for all of them rather than for the one that won.
A stem unrolled: 180 nodes at 136.78° with a rise of 0.013 circumferences. The 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.
Fig. 25 What an offset means in the arrangement rather than in the sequence, at the rise where the grid’s rows are deepest.

What a counter reports is a pair. What decides the survivor is a pair and a position on the rung the pair does not name. That is not a failure of counting; it is a statement about what counting is for. A spiral count is a robust, scale-free description of an arrangement, and its robustness is exactly its blindness: it is the same number over a range of geometries, which is what makes it worth measuring on a real plant and what makes it insufficient here.

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. 26 The packing the whole argument is about: the organs an organ touches are the members of its two contact families, at the two lags the pair names.

The next thing to do is not another sweep of this rung. It is to ask whether the family that survives is the one that did not lose a member — a reading the offset rule already suggests and the census cannot currently test, because it does not record which family the removed organ belonged to. That is one column, and it is the difference between a rule that fits and a mechanism that explains.

What links here

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

Shares its objects with

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

  • The shortest hop was a coin flip — both name ablation, control, falsifiability, honest limits, lattice, lattice offset, measurement, negative result, parastichy pair, the placement rule, rigid hop, rise, rung, underdetermination
  • One turn per survivor — both name ablation, falsifiability, honest limits, lattice, lattice offset, measurement, parastichy pair, the placement rule, rigid hop, rise
  • Three organs and no mirror — both name ablation, control, falsifiability, honest limits, lattice, measurement, parastichy pair, the placement rule, rise, rung
  • Two accounts of one number — both name ablation, honest limits, lattice, measurement, negative result, parastichy pair, the placement rule, rise, rung, underdetermination
  • A wreck has a short list — both name ablation, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair, the placement rule, rigid hop
  • Seven rises and two seeds — both name ablation, control, honest limits, lattice, measurement, parastichy pair, the placement rule, rise, rung

Named objects

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

AblationControlFalsifiabilityHonest limitsLatticeLattice offsetMeasurementNegative resultNodes per rungParastichy pairThe placement ruleRigid hopRiseRungUnderdetermination