How this site is made

The figure library — page 2

Every picture here is generated from code at build time. This is every generator, ordered by how many essays call it, each rendered at its defaults.
Cutting a square tessellation out of the plane, and gluing it upSearch cost in nodes, on a logarithmic scale, against how many periods of the tessellation the rectangle holds. The lower line is the rectangle cut out of the plane in the ordinary way; the upper is the same rectangle with its opposite edges joined, so that no crease is divided. Both search the same drawing under the same rule at the same vertices.the same drawing, cut out of the plane and glued upnodes, log scale, against periods across the sheet10100100010⁴10⁵1×12×23×34×4glued upcut outan open mark is a search that ran out of budget rather than a cost
The period cell of the Yoshimurathe Yoshimura drawn over the plane, with one period rectangle marked on it and a ring of its neighbours around it. The rectangle's edges are placed to miss every vertex, so identifying opposite edges can neither make nor destroy an interior vertex — there are 2 of them either way. one column wide and two courses high, because the courses alternate their offset.the period cell of the Yoshimuraone period, with its neighbours round it2 interior vertices in the cell12 crease pieces drawnperiod 0.167 × 0.289one column wide and two courses high, because the courses alternate their offsetthe cell is a rectangle of ordinary paper until somebody says its edges are one edge
The vertices a crease list does not haveEvery crease pattern here, read twice: once as the list of vertices and edges it is built from, and once as the ink on the page. The bar is how many vertices the second reading has to invent, which is how many places two creases cross with nothing recorded there.the bar is the vertices the drawing has and the list does notThe preliminary base09 listed · panels closeThe Miura fold035 listed · panels closeThe square twist016 listed · panels closeThe hexagon twist022 listed · panels closeThe Yoshimura pattern045 listed · panels closeFold and cut — the triangle011 listed · panels closeThe tapered corrugation040 listed · panels closeThe waterbomb tessellation041 listed · panels closethe square grid, assembled064 listed · panels closethe triangular grid, assembled1282 listed · panels 1.73 apartthe honeycomb, assembled1884 listed · panels 2.00 apartthe rhombille tiling, assembled12138 listed · panels 1.86 apartthe elongated triangular tiling, assembled576 listed · panels 1.73 apartevery pattern with a bar has panels that cannot be placed, and every pattern without one places exactly
How far a hand travels to fold each printed patternThe total length of crease in every pattern this site prints at true scale, in millimetres at the size it is printed. It runs from 258 mm to 6,679 mm, and it does not rank the patterns the same way counting their creases does.the bar is millimetres of crease at the printed sizea pattern with more creases is not always a pattern with more folding in itThe preliminary base724 mm8 creases · printed at 150 mmThe Miura fold1,049 mm38 creases · printed at 170 mmThe square twist704 mm12 creases · printed at 150 mmThe hexagon twist916 mm18 creases · printed at 150 mmThe Yoshimura pattern2,380 mm86 creases · printed at 170 mmFold and cut — the triangle258 mm6 creases · printed at 150 mmThe tapered corrugation1,057 mm45 creases · printed at 160 mmThe waterbomb tessellation2,290 mm76 creases · printed at 160 mmsix point seven metres of crease on a sheet seventeen centimetres across
What each machine can reachFor three one-dimensional crease patterns, the number of mountain-and-valley assignments that fold flat at all, and the number each kind of folding machine can actually reach. Every bar is a separate search: the top one over stackings, the next three over sequences of folds, the last over rewritings of the segment lengths.evenly spaced — 4 creasesany flat folding16 of 16some-layers16 of 16all-layers16 of 16one-layer2 of 16crimping only6 of 16one short segment — 4 creasesany flat folding4 of 16some-layers4 of 16all-layers0 of 16one-layer2 of 16crimping only4 of 16uneven — 4 creasesany flat folding8 of 16some-layers8 of 16all-layers0 of 16one-layer2 of 16crimping only0 of 16a machine that takes fewer layers is weaker, not more patientthe paper is joined, so what it declines to hold it also cannot move
The Miura foldA grid of identical parallelograms. The assignment is the whole trick: the horizontal creases alternate by row, and the vertical ones change assignment every time they cross a row, so each vertex ends up three of one and one of the other rather than two and two.at every vertexthree of one, one of the other15 interior vertices, all identicalwhat the sheet gainsone degree of freedom, not manyit opens and closes in both directions at oncea negative Poisson's ratio22 mountain and 16 valley creases · 6.2 sheet-widths of foldingmountainvalleyraw edge
Miura fold — sheet 170×106.83 mm — 22 mountain, 16 valley, 1049.4 mm of crease
The same parity, with nowhere to put itThe same creases on a square of paper and on a loop of paper. On the left they meet at one interior vertex, which carries the parity and which every theorem in the subject inspects. On the right the middle has been removed, that vertex is gone, and the parity is still there — in the panels, where nothing local can see it.a disc, with a vertexa ring, with noneone interior vertex, 3 creases at itodd degree, so they do notno interior vertices at alland the panels still do notboth refuse: two routes round the sheet leave a panel 1.87 sheet-widths apart
More sides is not more paperThe area of the largest regular polygon of each number of sides that fits inside a square sheet. The square and the octagon share the sheet's own symmetry and do well by it; the polygons between and after them do not, and the sequence goes up and down rather than up.sidesshare of the sheet the largest one usestilt346.4%15.00°4100.0%45.00°567.4%9.00°669.6%15.00°772.9%6.43°882.8%22.50°975.1%5.00°1075.3%9.00°1176.3%4.09°1280.4%15.00°the 8-sided polygon is the peak, and every one of the 4 polygons after it does worse
The seven ways to specify a foldThe Huzita–Hatori axioms: every fold that can be specified by bringing existing points and lines into coincidence. The list is complete — six were catalogued in 1991, the seventh in 2001, and no eighth exists. The sixth is the one a compass cannot reach.axiom 1through two pointslinearaxiom 2point onto pointlinearaxiom 3line onto linelinearaxiom 4through a point, square to a linelinearaxiom 5point onto a line, through a pointquadraticaxiom 6two points onto two linescubicaxiom 7point onto a line, square to a linelinearthe degree each axiom can solve — one of them is why paper beats the compass
The smallest sector decidesTwo assignments of the same four creases. Both satisfy Kawasaki and Maekawa. The left one folds; the right one does not, because the strictly smallest sector has the same assignment on both sides and the paper either side of it has nowhere to go.MVMM40°foldsopposite across the small sectorMMVM40°does not foldthe same on both sidesboth satisfy Kawasaki and Maekawa — the angles and the counts are identical
Box pleatingDesigning on a grid, with every crease running along a grid line or at forty-five degrees to it. It gives up the efficiency of a free circle packing and gains something worth more for complex work — the creases meet where they are supposed to, and the errors do not accumulate.16 × 16 gridevery crease on a grid line, or at 45°which is why a 64-grid design can be folded at allmountainvalley
Growth is a change of metric, and a metric decides a curvatureThe linear growth factor against radius, and the Gauss curvature that metric forces. Nothing about a material enters either panel: given how much each part of the sheet grew, the curvature is determined, and a curvature that is not zero is a sheet that cannot lie in the plane.00.20.40.60.8100.511.5radius on the flat sheetgrowth factor Ωhow much each ring grew00.20.40.60.81-2-112radius on the flat sheetcurvature Kclosed formthe curvature that forcesgrown more at the rim · K(0) = −4a = -2.40