Crown line — where it appears
Named by 31 essays across 8 fields — each of them below, with the objects they name alongside it.
A cloth has an outside
Every quantity in this collection is a property of the inside of a fabric — a crimp, a cover, a hole, a fibre count. None of them says where the cloth stops. The outside is a height field the draft computes, its crowns stand at two different levels, and which of the two is higher decides what the cloth touches the world with.
The curve that says what a cloth touches with
Take a cloth's surface and ask what fraction of the plan lies within a given depth of its highest point. The answer is one curve, it answers every question of the form what does this touch, and its behaviour at the top is decided by a single bit of the draft — whether the longest float is one crossing or more than one.
Two drafts of twenty-two thousand
Every four-by-four draft there is, measured by how much horizontal crown line its surface carries. Two of them carry none — the plain weave and its translation, and nothing else in the catalogue — and the quantity turns out to be smallest for the most balanced cloths and largest for the most one-sided, which is the opposite of what a float count suggests.
A figure shows by its shine, not its step
A damask is one cloth in one colour and its pattern is plainly visible. This collection attributed that to the step in its surface — fifty micrometres of relief, computed from the interlacing rates. The step is real and returns almost no light. What makes the figure visible is that its crowns run at right angles to the ground's, so the two trade places when the cloth is turned.
A jersey has two surfaces
The face of a plain knit shows the legs of its loops, which run along the wale; the back shows the heads and feet, which run across it. So the two faces carry their crowns at right angles — the same situation as a damask's figure and its ground, in a fabric with no warp, no weft and no float.
A pile is the only surface with no crowns
Every other fabric touches on the tops of curved threads, so its contact vanishes as the load goes to zero and the pressure on what is touching rises without limit. A cut pile touches on flat ends left in one plane by a blade — so its contact is finite at no load at all, its pressure concentration is bounded, and it is the only fabric whose abrasion mass loss is an honest measure of its damage.
A shadow stripe is two twists
A cloth striped in one colour, where the stripe is visible only because alternate bands are spun the other way round. The pattern is carried entirely by which way the fibres lie on the yarn's surface, and it disappears when the light moves.
A tone ramp is a valley, and the satin digs it
A shading's tone is exact and its lustre is measured; its thickness is neither, and nobody specifies it. A firmer weave is pressed harder at every crossing and finishes thinner, so an eight-end shading sinks eighty-four micrometres between its ends and its midtone — about a third of the cloth's whole thickness, on every cloth tried. Build the same chain on a twill instead of a satin and the sag is exactly nothing.
Raising moves the surface onto the hairs
A raising machine pulls fibre ends up out of the floats, and what a finger or a light then meets is not the cloth's surface at all but a layer of loose fibre standing above it. The criterion for which cloths can be raised is the same criterion, exactly, that decides which cloths have crown line — so raising spends the surface that would have made the fabric shine.
A cloth loses its strength before its mass
Rub a fabric and it sheds material from all over its surface, but it sheds it from every thread at the same place — and a thread breaks at its thinnest place. So the strength gone is always several times the mass gone, the ratio is computable from the bearing curve, and it is worst for the weave whose crowns are points.
A coating fills the crowns before it bridges the holes
A film does not sit on a cloth, it fills it — and the volume it has to supply to reach a level is the integral of one minus the bearing area. Burying an ordinary sheeting's crowns takes 185 grams a square metre, which is more than the cloth weighs, and the whole of the weave's influence is spent in the first ten of them.
A light touch never reaches the crowns
A plain weave touches at points and every other cloth touches along lines, and the difference is an exponent rather than a factor. It is a real result about a real surface, and at the pressures a fabric is actually touched at, nothing ever reaches that surface.
A float reflects into a line
A cylinder cannot return a beam to a point. Its normals sweep the whole half-turn across it and nothing at all along it, so a straight thread throws light into a fan — seen as a highlight lying along the thread, exactly as long as the length of thread that is straight. The lobe of a satin is twice as narrow along the thread as across it; the lobe of a plain weave is exactly round.
Lustre is a length times a width
The specular area of a cloth factors exactly: a length of crown line, which the draft supplies, times a width of section within the tolerance, which the yarn and the finish supply. Neither factor knows anything about the other, and over the four-by-four catalogue the first alone spans a factor of sixty.
A calender buys the width
Press a cloth and its lustre multiplies by twenty-four. None of that comes from the length of its crowns, which moves by six per cent; all of it comes from their width, because a flattened section has a plane on top of it and a plane has one normal rather than a fan of them. The arithmetic refuses to put any of the gain in the other factor.
A cloth compresses along its own bearing curve
A fabric's pressure–thickness curve is always fitted with an empirical power law and the exponent is reported without explanation. It is not empirical. At light loads it is two thirds for any weave carrying a float and one half for a weave carrying none, and the two numbers come out of one line of algebra with nothing fitted in it.
Turn the cloth and the shine changes hands
A warp crown's normals all lie in the plane across the warp and have no component along it, so a warp float can only mirror light that arrives from across the warp. Turn the cloth a quarter turn and the weft takes over. That is the whole of shot silk — a geometric effect with no dye that changes and no interference in it.
A crepe is flat in its draft and not in its surface
A crepe weave is chosen by pushing the draft's correlations as flat as they will go. That criterion turns out to tie: on the base this collection uses, 4,416 of the 5,040 rearrangements reach the floor. Sixteen of them additionally spread their crown line perfectly evenly — and the crepe actually drawn is not one of the sixteen.
A hair layer veils a highlight
An eight-end satin's shine swings by a large factor as the cloth is turned, because a straight thread's normals lie in the plane across it. Put fibre ends on it and the swing disappears — not because the hairs block the light, which changes no contrast at all, but because they return light of their own that has no direction in it.
An unbroken line is not a clean one
A line of colour has two boundaries and neither is straight, in any weave there is. The thread at the edge must go under somewhere, and where it does the edge retreats to its neighbour — so the boundary steps, and by exactly one thread less than the narrowest unbroken line the weave draws. Over 22,874 drafts there are three widths and three swings and no draft anywhere else, and widening the line past its narrowest unbroken width leaves the edge precisely where it was.
The census counted two systems and a surface has one
Two drafts of twenty-two thousand touch at points, and the two are the plain weave. That is a count of the crown line both systems carry, and a bearing curve sees one: a plate meets whichever crown stands higher and meets nothing else until it has sunk past the step. Counted the way a surface is read, 494 drafts touch at points rather than two — and which 494 depends on a crimp division already called a convention rather than a measurement.
Four drafts in five have no path along their own crowns
A 2/2 twill and a 2/2 hopsack carry exactly the same length of bearing crown line, which the surface census noted and could not explain. One of them is a ridge running diagonally across the cloth without a break; the other is a field of square islands with no path between them. Counted over the whole catalogue, 4,016 of 22,874 drafts have a crown path that reaches the far side, 1,616 have one in both directions, and 130 have crowns with no neighbour at all.
No cloth shines under a sky
Every specular figure on this account is drawn at a tolerance of two degrees, which is a stand-in for how wide the source is. Sweeping it says something the account has not: the contrast between a floated weave and a plain one is inversely proportional to the source's angular size, exactly, because a float keeps a crown line as the source narrows and a plain weave has only turns. A satin outshines a plain weave by 177 under the sun's disc, by 22 under a small lamp, and by exactly nothing at sixty degrees.
A ridge in the matrix is not a ridge in the cloth
A 2/2 twill's crowns join into a ridge across its matrix and a 2/2 hopsack's are islands, so a thin film on the twill should be continuous from the first gram and on the hopsack a scatter of patches. Laid on the cloth's own surface rather than its matrix, both films are patches — the twill's ridge crosses from one end to the next, and between two ends lies the gap the sett leaves. On a sheeting both join at the same depth, 116 grams into the 186 that flatten the face, and the weave's whole influence is a window of up to 27 grams at the setts where it opens at all.
A calender's best cloth is the one its nip fills
A calender's lustre is a length of crown line times a width of plateau. A closer cloth has more crown line and less room to widen each thread into, and the product was expected to peak at some interior cover that would move with the weave. It does not peak at all on the cap alone — per unit of crown line it falls all the way from the most open cloth. The peak is made by the nip: a nip that flattens by f has one best cloth, the one it exactly fills, at a cover of d over the flattened width, and there the lustre is (f − 1)/f. No yarn, and no weave, moves it.
A room lights a satin at the harmonic mean of its lamps
A satin outshines a plain weave by a factor inversely proportional to the width of the light, which is a clean law for one source and says nothing about a room. A room has a lamp and a window at once. Sum each source's highlight and the average falls out by itself: the room behaves as a single source whose width is the harmonic mean of its sources' widths, weighted by the power each supplies. The harmonic mean is ruled by the narrowest source, so a small lamp carrying a tenth of the light more than doubles the contrast a large window gives.
A lamp off the mirror lights a satin only across its floats
Every source in the account of a room was a source the viewer sees mirrored in the cloth. A lamp off to one side lights the cloth too, and which facets it reaches depends on which way it is off. Displaced across a satin's floats it is caught by the float's own curve and adds contrast like any lamp on the mirror; displaced along them by more than twice its own width it reaches only the turns, and the satin comes out a quarter as bright as plain weave.
A satin mirrors the top of the sky
A uniform source sixty degrees wide leaves every weave reflecting the same share of its face, and that was read as saying no cloth shines under a sky. A real sky is not uniform. An overcast one is three times as bright overhead as at the horizon, and it stands over a ground darker than itself. Every facet of a cloth mirrors one direction, and a satin's facets mirror the top of the dome while a plain weave's mirror the horizon and the ground — so seen from above, under cloud, an eight-end satin still sends back a third more sky.
A float fades late and hard, a crossing early and soft
Wear a ring-dyed face flat and the white arrives where the cut first passes the ring at a crown, which is the same depth for every weave. What differs is how much cloth has gone by then and how fast the white spreads after. A plain weave's crowns are points, cut through by almost nothing: it shows white after a fifth of a per cent of its thread and never shows much. A twill's floats are lines, cut along their length: a 3/1 twill shows nothing until more than one per cent has gone, then whitens faster than any plain weave can, 39 per cent of its face by a tenth worn against plain's 24. Denim's high-contrast fade is a float's; chambray's soft one is a crossing's.
A crease across a twill fades in dashes
A garment is not worn flat. It is worn along its folds, where the ridge of a crease stands out and is rubbed first, so the fade follows the crease. On a ring-dyed 3/1 twill a crease running along the warp bares the cores of the floats that lie under its ridge, float by float, and reads as a white line broken only where each float dives: at fifty micrometres of wear, 83 per cent of its length is white, in runs of 1.7 millimetres. The same crease across the warp meets every float at one point and reads as a row of dots, 31 per cent white in dashes of 0.15 millimetres, one end wide. It bares much the same core. A plain weave's creases are dashes whichever way they run.
A crease along the twill fades as one line
A crease along the warp of a ring-dyed 3/1 twill fades as broken lines a float long, and across it as dashes one end wide. Turn the crease to the twill's own diagonal and it fades as a single white line with no break in it at all: the fold meets the crown of one end's float, then the next end's one pick along, then the next, and every crown it meets is at the same place in its float. It is the one direction in which the weave and the crease line up — and two degrees off it the line breaks into strokes whose length is a vernier's.
Named alongside it
The objects these essays reach for when they reach for this one.
Bearing curveLustreSpecular areaSurface heightFloatPlateauFloat lengthCensusCloth thicknessSpecular reflectionAbrasionCatalogue