Setting and geometry

A warp jams where its threads are thickest

The closest a cloth can be set is decided by its worst pair of neighbours, not its average thread — and the worst pair depends on how many pairs there are. The same yarn in a wider loom jams sooner, which makes a jammed sett a property of the machine as well as of the yarn.

Worth reading first: How close can threads be set · A cloth is a population, not a thread · The reed is not the sett.

The maximum sett of a yarn is one of the oldest computations in the trade. Threads cannot overlap, so the closest they can lie is when they touch; a diameter gives a jammed spacing, and the jammed spacing gives a sett. This collection has done it too, with a proper section geometry rather than the flat-disc version, and got numbers that behave sensibly against the setts weavers actually use.

Except that they behave sensibly by being much too high, and the gap is always explained away the same way — a cloth at its geometric jam cannot be woven, the shed will not open, the reed will not clear, so weavers set below the maximum by a margin that experience supplies.

Some of that margin is not experience. It is arithmetic, and it can be computed exactly.

Where a muslin's warp jams, over 40 ends. 40 ends drawn at their own diameters, with every neighbouring pair's combined width plotted beneath. A cloth cannot be set closer than its threads will lie, and the pair that decides that is not the average pair — it is the widest one anywhere across the warp, which here is ends 8 and 9 at 205 µm apiece against a mean of 167 µm. Over the 2000 ends of a real warp rather than the 40 drawn here the worst pair is 42% above the mean, and it goes on growing with the width of the cloth: the same yarn in a wider loom jams sooner. The naive estimate that treats every window as an independent try overstates it by 0.48%, which is small enough to say that the overlap between neighbouring windows is not what is going on here.
Fig. 1 Forty ends at their own diameters, with every neighbouring pair’s combined width plotted beneath. Two neighbours touch when their two radii reach the spacing, so what decides whether this warp can be beaten up at a given sett is the tallest bar — not the average one, and not the one in the middle.

The claim

A jammed sett is an extreme value, so it depends on how many threads there are. A warp of a hundred ends of ordinary cotton jams thirty per cent above its mean diameter; one of ten thousand ends of the same yarn jams fifty per cent above it.

That is an uncomfortable statement, because a jammed sett has always been quoted as a property of the yarn. It is a property of the yarn and of how wide the cloth is, and the second is not a small correction: doubling a loom’s width moves the jam by three or four per cent, and the range from a ribbon to a broadloom moves it by twenty.

The argument

Two ends touch when the sum of their radii reaches the spacing between them. The spacing is fixed — set by the reed and by the take-up, and not the same thing as the sett — so what has to fit is the sum of two neighbouring diameters, and what decides whether a cloth can be woven at a given sett is the largest such sum anywhere across the width.

That is an extreme of a moving sum, and three things follow immediately.

It grows with the width, because more pairs is more chances. The growth is logarithmic and therefore slow, which is the only reason the trade’s practice of quoting one figure per yarn works at all.

It falls with the length of the run, because a run averages its own members. The thickest single end in a warp of a thousand is 61 per cent above the mean; the thickest adjacent pair is 40 per cent above; the thickest run of four is 26 per cent above. A quantity decided by a longer run is a quantity decided by a partly averaged population, and the averaging takes the tail out.

And it is what the reed and the cloth each ask that differ. The cloth jams pairwise: two neighbours touch, or they do not. A reed dent holds two, three or four ends together and asks whether the whole group will pass through a fixed slot — so the reed’s constraint is a run of four, which is a full fourteen points gentler than the cloth’s. The reed is not the binding constraint on a variable yarn, which is the opposite of what a weaver watching threads chafe in the dents would guess.

How far above its mean diameter a warp jams, against how wide it is. A cloth cannot be set closer than its threads will lie, and what decides that is not the average thread — it is the worst run of them anywhere across the width. Three runs are plotted: the single thickest end, the thickest adjacent pair, which is what decides whether two neighbours touch in the cloth, and the thickest run of four, which is what has to pass through one dent of a four-ended reed. Every one of them climbs with the number of ends, because an extreme is a question about how many tries there were: at CV 15% the worst pair in a hundred ends is 30% above the mean and in ten thousand it is 49%. The longer the run, the lower the curve, because a run averages its own members — which is why the reed is a gentler constraint per thread than the cloth is.
Fig. 2 The three runs against the number of ends. Every curve climbs, because an extreme is a question about how many tries there were, and the curves are ordered by how much averaging each run does. The gap between the pair and the run of four is the difference between what the cloth asks and what the reed asks.

Why the pair and not the thread

The choice of run length is the one modelling decision in this essay, and it is worth defending because the answer moves by twenty points depending on it.

A single thread cannot jam. Jamming is a statement about two things not fitting into the room between them, so the smallest object that can jam is a pair, and the quantity that has to clear the spacing is the sum of two radii — one from each of two different threads. The thickest single end in a warp is a fact about that end; it becomes a fact about the cloth only when the end beside it is asked as well.

That is why the pair curve is the one to read for the cloth, and it is also why the pair curve sits well below the single-thread curve: a pair is already a small average, and the thickest end in a warp is very unlikely to have the second-thickest beside it. The extreme of a sum of two is not the sum of two extremes — an identity that does hold for a thickness under a presser foot, because there the two maxima are over different populations, the ends and the picks, and here they are over the same one.

Two objects with the same name and different arithmetic, which is exactly the trap this collection keeps recording: read the bodies, not the names.

Where a muslin's air goes, as the cloth is set closer. A permeability computed from the average hole says nothing about which holes the air uses, and once the holes have a spread the answer is: not many of them. Two curves, both over the same population of holes — the share of the flow carried by the widest tenth, and how few of the holes carry half of it. At 16 ends per centimetre the cloth is nearly democratic: the widest tenth takes 12% and half the air needs 45% of the holes. At 44 the widest tenth takes 53% and half the air goes through 8.8%. Both inputs move together as the cloth closes — the spread in the holes rises because the spacing is fixed and the diameter is not, and the exponent rises because the pressure drop stops being inertial — so the concentration rises faster than either.
Fig. 3 Where a muslin’s air goes as it is set closer. The jam does not arrive everywhere at once: it arrives first where the threads happen to be thickest, so the cloth is part-jammed over a range of setts rather than open up to a number and shut after it.

What was counted, and how

Warps of the stated width are drawn from a lognormal at the yarn’s coefficient of variation, every run of the stated length is summed, and the largest is kept — forty warps at each width, so that the number reported is an average of forty worst cases rather than one.

The simulation is checked against the order statistic that would apply if every window were an independent draw. It is not one: consecutive windows share all but one of their terms, so the effective number of tries is smaller than the number of windows and the independent estimate should sit above the simulation. It does, by 0.3 per cent — small enough to say plainly that the overlap between neighbouring windows is not what is going on here, and that the whole effect is the extreme rather than the correlation.

That check is worth its cost precisely because it came out uninteresting. The alternative was a paragraph of hedging about dependence in a moving sum, which would have been true, unquantified, and much larger in the reader’s mind than the third of a per cent it is worth.

What it does to the setts this collection has quoted

Every jammed sett in this collection was computed from a mean diameter, so every one of them is a sett a warp of one thread could reach.

How much a moment exceeds its own mean, at each spread. A quantity going as the kth power of a varying thread does not come out at the kth power of the mean thread. For a lognormal the excess is a single closed form — (1 + CV²) raised to k(k−1)/2 — so the second moment is up by the square of the CV and nothing else, and the fourth is up by that to the sixth. At the fifteen per cent an ordinary staple yarn reaches, the ratios are 1.0225, 1.0690, 1.1428 for k = 2, 3 and 4. The dashed curves are a normal with the same mean and CV, which is what a laboratory quotes and what a diameter cannot actually have, since a normal diameter can be negative: the two laws agree to a few parts in a thousand across the whole range a yarn occupies and part company in the tail, which is exactly where the extremes this family also computes live.
Fig. 4 Why the effect is a moment rather than a mean. The jam is set by the thickest threads and the thickest threads are the tail of a distribution, so what decides it is a higher moment of the spread — and higher moments rise far faster with the spread than the mean does.

The correction is a multiplication and it is uncomfortably large. A cloth of two thousand ends at a fifteen per cent yarn cannot be set within forty-three per cent of the sett its mean thread allows, because somewhere across that width there is a pair that will not go. In practice a weaver stops before that, because a cloth right at its jam cannot be beaten up and the shed will not clear — but the arithmetic says that a substantial part of the traditional margin is not craft caution at all.

And it explains a fact about fine yarns that is otherwise odd. A combed, well-made yarn is more even as well as finer, and its lower coefficient of variation moves its jam closer to its geometric value. So two yarns of the same count but different evenness have different maximum setts — the even one can be set closer — even though every geometric quantity in a specification for them is identical. That is a real difference in what can be made, priced by a number that appears on the yarn’s delivery note and never reaches the cloth’s.

What a 15% spread does to each of this site's own quantities. Seven quantities this collection computes from a thread's diameter, each pushed through a population of threads whose mean is a muslin's and whose coefficient of variation is 15%, and reported as the excess of the population's average over the value the average thread gives. The order is decided by one thing: the curvature. A cover factor is linear in the diameter and is unaffected at any spread whatever — the zero in this table is exact and is the control on the method. A mass goes as the square and is 2.25% high; a bending rigidity goes as the fourth power and is 14.3% high. Every convex quantity is under-reported by the mean thread and no concave one is over-reported by less, which is Jensen's inequality doing the only thing it does.
Fig. 5 Where the jam sits among the other quantities a spread touches. It is not on this chart, and that is the point: everything here is a bias on an average, correctable once and for all by a factor. A jam is not — it is an extreme, and its correction depends on how much cloth is being asked about.

The weft has a far larger population than the warp

There is an asymmetry hiding in this that no geometric account of jamming can contain, because it is about counting rather than about shape.

A warp has as many ends as the cloth is wide: two thousand for an ordinary shirting, ten thousand for a wide sheeting. A weft has as many picks as the piece is long — a fifty-metre piece at twenty-two picks per centimetre has a hundred and ten thousand of them, and every consecutive pair of them is another chance at a jam.

So the two directions are drawing their extremes from populations that differ by a factor of fifty, and the excess follows:

pairs available jam, above the mean
warp of a 1.5 m shirting 2,000 43%
weft of a 50 m piece of it 110,000 59%

A square-set cloth is not symmetric in this respect at all. The two systems have the same yarn, the same mean diameter and the same nominal sett, and the weft’s worst pair is a sixth further above the mean than the warp’s, purely because there are more picks in a piece than ends across it.

What saves the weft is that its jam is not a hard stop. A pair of thick picks cannot refuse to be woven; they are simply beaten up against more resistance, so the beat-up takes them a little less far and the pick spacing opens locally. The warp has no such escape: an end that will not pass its neighbour has to break, or chafe, or stop the loom. The same arithmetic produces a fault in one direction and a variation in the other, and which of the two it is depends entirely on which system is free to move.

The evenness that buys a sett

Because the jam sits at a fixed number of standard deviations above the mean, it moves in proportion to the spread — so evenness converts directly into how close a cloth can be set.

A bundle is weaker than the threads it is made of. Threads pulled in parallel do not break together. The weakest goes first and hands its load to the rest, which are now carrying more than they were, so the bundle's peak load is reached before every thread is at its own strength. With a load per surviving thread of x carried by the fraction that has not yet broken, the bundle's strength per thread is the largest value of x(1 − F(x)) — Daniels' maximum, which for a lognormal at CV 10% is 0.8024 of the mean thread, reached with 95% of the threads still unbroken. A simulated bundle that knows none of that arithmetic sits above the limit at every finite size — its strength is a maximum over the sample it happens to have drawn — and closes on it as the bundle grows: 0.816, 0.808, 0.805 at the last three sizes. The scatter falls the other way, from 9.7% at one thread to 0.5% at 1600.
Fig. 6 A very even warp, which is the evenness that buys a sett. With little scatter the thickest place is barely thicker than the mean, so the jam arrives where the arithmetic says it should — and the several ends per centimetre a mill gains from a better yarn are gained here rather than at the loom.
yarn CV jam, above the mean diameter
8% 21%
12% 33%
15% 43%
20% 61%

A combed yarn at eight per cent can be set within a fifth of its geometric jam; a coarse carded one at twenty cannot come within three fifths of it. Both yarns have the same mean diameter and the same count, so nothing that appears in a construction specification distinguishes them, and the difference between them is a third of the available sett range.

That is a large enough number to change what is worth buying. The premium on an even yarn is usually justified by appearance — fewer thin places, a cleaner surface, less barré — and appearance is a matter of taste and of light. This is not: it is the difference between a cloth that can be made and one that cannot, at a construction the buyer has already specified.

Why a sample loom lies, and by how much

The width dependence is stated above as a curiosity about broadlooms. It has a much more common consequence, and it is one that every product-development department meets and attributes to something else.

The extreme of a large sample sits about √(2 ln n) standard deviations above the mean, and the standard deviation of a pair’s mean diameter is the yarn’s own coefficient of variation divided by √2. So the excess is

CV × √(ln n) to a good approximation,

which for a fifteen per cent yarn over two thousand pairs gives 41 per cent against the 43 the simulation returns — close enough to trust the scaling and not the third figure, the gap being the lognormal’s own skew, which a Gaussian estimate cannot carry.

Now put two widths through it. A thirty-centimetre sample blanket at the same sett has about 450 ends and jams 37 per cent above its mean diameter. The 1.5-metre production cloth has 2,250 and jams at 42.

Five points of sett, between a sample and the production run of the identical construction in the identical yarn.

That is a familiar and thoroughly annoying industrial fact: a construction proves out on the sample loom, goes to production, and chafes. The usual suspects are the loom, the beam, the sizing and the humidity, all of which are plausible and all of which get investigated. The arithmetic says a share of it is neither — it is that a wider warp is a larger sample of the same yarn, and a larger sample has a worse worst pair.

And the effect cannot be sampled away. Weaving a longer trial on the narrow loom does not help, because the warp’s population is set by its width and not by its length. The only honest trial of a warp’s jam is a trial at the production width.

What each doubling costs

Because the excess goes as the square root of a logarithm, its increments are regular and shrinking. Differentiating, a doubling of the width adds

What a 15% spread adds to a muslin's air, against its sett. Two multiplications, one after the other. A hole is the spacing less the diameter, and the spacing does not vary — so a yarn at 15% leaves holes at 5% in an open cloth and 61% in a close one, the subtraction amplifying the spread by d/w. Then the exponent multiplies it again, and the exponent itself rises from 2.09 to 3.97 as the cloth closes. The result is that a permeability computed from the mean thread is 0.3% low at 16 ends per centimetre and 204% low at 48 — the direction of the standing discrepancy between what geometry predicts for a close fabric and what a permeameter reads.
Fig. 7 The excess in the gaps, which is what each doubling is spending. Doubling the width doubles the number of ends and moves the thickest place further into the tail, so each doubling costs a fixed fraction of a sett — and the cost is the same fraction every time.

CV × ln 2 ÷ (2 √(ln n))

which at two thousand ends and a fifteen per cent yarn is about two points of sett margin, falling to one and a half at ten thousand.

So the penalty for width is real, bounded, and front-loaded: the step from a ribbon to a shirting costs more than the step from a shirting to a sheeting, and a mill that already weaves wide is not being punished much further for weaving wider. That is a comfortable shape, and it is the reason the trade’s habit of quoting one jammed sett per yarn survives at all — the quantity it ignores changes by a couple of points across the whole range of looms in use.

The same expression run the other way says what evenness is worth against width. Since both terms multiply, a yarn one point better in CV buys back about the same margin as halving the loom’s width, at ordinary values. A mill choosing between a finer-spun warp and a narrower cloth is choosing between two ways of buying the same number, and only one of them costs anything per metre.

And the weft’s is a running total

The pick population grows with the piece rather than being fixed by the machine, which gives the weft’s version of the same statement a different and slightly unnerving shape.

A five-metre trial length carries 11,000 picks and its worst pair sits 46 per cent above the mean. The fifty-metre production piece carries 110,000 and reaches 51.

So the weft’s jam gets worse as the piece is woven, in the sense that the worst pair encountered so far keeps climbing — logarithmically, so slowly, and without limit. A trial length cannot demonstrate the absence of a fault that only the tenth of the run is long enough to contain, and the growth is not a matter of anything wearing out.

That is a genuine limit on what a trial can prove, and it is arithmetic rather than pessimism.

Where the model stops

A thick place is not a whole thread. The variation used here is between ends, and a real yarn also varies along its own length, so the pair that jams does so at one place down the piece rather than everywhere. A cloth can be woven past its pairwise jam if the jam is momentary — the beat-up simply pushes a little harder for a few picks — and what that costs is a local disturbance in the pick spacing rather than a stoppage. Nothing here prices that, and it is the reason the number above is a bound rather than a prediction of where a loom stops.

The threads are treated as independent. Neighbouring ends come from different bobbins and are genuinely independent; but a yarn’s own thick places recur at the spinning frame’s period, so one end’s thick places are not independent of each other. That does not affect the pairwise jam, and it does affect how often it occurs down the piece.

The section is circular and the diameter is Peirce’s. A flattened thread jams at a different place, and a thick end under a hard beat-up flattens more than its neighbours, which relieves exactly the pair that was binding. So the extreme computed here is the extreme of an unyielding population, and a real warp buys some of the margin back the moment it is pressed.

And nothing here is about the loom’s other limits. A shed that will not clear, a reed that chafes, a warp that sheds fibre: those are the reasons a weaver gives for setting below the maximum, all of them real, and none of them touched by this argument. What is claimed is only that the arithmetic contributes a share of the same margin, and that its share is computable while theirs are not.

The generalisation

A limit that has to hold everywhere is an extreme, and an extreme is a question about the size of the population. That is the general shape, and it turns up wherever a system fails at its worst point rather than at its average one: the narrowest place in a pipe, the weakest link in a chain, the shallowest patch of a channel, the thinnest section of a casting.

The diagnostic is the same one this ladder keeps returning to. Ask whether the number would change if twice as much of the same thing were included. A mean would not. A jam would, and does, and the arithmetic of how fast is the difference between a specification that transfers between looms and one that does not.

The second lesson is that averaging is a design variable. The reed jams over a run of four and the cloth over a run of two, and that single difference is worth fourteen points of margin. Wherever a constraint can be arranged to apply to a group rather than to an individual, the tail of the population stops deciding the answer — which is why a dented reed is a kinder machine than its geometry suggests, and why the fix for a marginal jam is sometimes to change the denting rather than the sett.

Who found it, and when

The geometric jam is Peirce’s, from 1937, and everything since has refined the section rather than the argument. That real setts fall well short of it is universally known and universally attributed to weavability.

The extreme-value part appears not to have been written down for a warp, though the ingredients are old: yarn evenness has been measured since the 1940s, and the growth of a maximum with sample size is elementary. What makes it worth the arithmetic here is the direction of the surprise — not that the jam is lower than the geometry, which everybody knows, but that it depends on the width of the loom, which nothing in the geometry can express.

Where the ladder goes next

The other two extremes in this ladder are the same argument with the maximum somewhere else: a thickness gauge reads the highest crossing under its foot, and at the other end of the distribution a bundle of threads breaks well below its mean thread.

Sideways, a warp set near its jam is a warp whose holes are nearly shut, and the holes at that point vary far more than the threads do — which is where most of a close cloth’s air comes from.

What links here

Computed from the collection rather than 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 naming at least two of the same things, that neither author linked.

Named objects

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

Coefficient of variationDentingJammingOrder statisticPopulationReedSettYarn diameter