Shine — the series
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.