The other systems

A drawn fold has a phantom

A Necker cube has two readings and so does a drawn fold, and the fold's second reading is not the supplement of the first. The drawing fixes each plate edge's component in the picture and leaves its component along the ray free up to a sign; a reflection identifies two of the four sign pairs, so there are exactly two plates — and a hundred-degree fold reads as eighty-seven as well.

Worth reading first: The drawing does not say which corner is nearer · The view that makes a line a point · No view draws a curved plate true.

The drawing does not say which corner is nearer is the field’s account of the Necker reversal: a parallel drawing of a box has no depth cue in it, so a corner can be read as the near one or the far one, and the two readings are two different solids drawn identically.

That essay is about a solid. The drawing office draws sheet, and a sheet’s version of a corner is a fold — two plates hinged along a line, at some dihedral angle. It has a reversal too, and the reversal behaves differently.

One drawing, two plates: 100.0° and 86.6°Two plates hinged along one line at 100°, drawn orthographically. The drawn angle between the two plate edges is 94.35°, which is neither reading. The drawing fixes each edge's component in the picture and leaves its component along the ray free up to a sign, and an overall reflection identifies two of the four sign pairs — so there are exactly two plates consistent with these marks, at 100.000° and 86.554°. This is the Necker reversal moved from a solid's corner to a sheet's fold, and the second reading is not the supplement of the first: 180 − 100 is 80°, which is not on the list.one platethe otherthe hingedrawn at 94.3° · reads as 100.0° or 86.6°an orthographic drawing of a foldtwo readings, 13.4° apart
Fig. 1 Two plates hinged along one line at a hundred degrees, drawn orthographically. The drawn angle between the two plate edges is neither reading, and there are exactly two plates consistent with the marks.

Where the two readings come from

Take the hinge along the xx axis and the two plate edges perpendicular to it, of known length LL. A parallel drawing fixes each edge’s component in the picture: two numbers per edge, read straight off the paper.

What it does not fix is the component along the ray. But it is not free — the edge has length LL, so

along the ray  =  ±L2drawn2\text{along the ray} \;=\; \pm\sqrt{L^2 - |\text{drawn}|^2}

and there are two choices per edge, so four sign pairs.

An overall reflection — turning the whole plate over, which is the same drawing seen from behind — flips both signs at once, so it identifies (+,+)(+,+) with (,)(-,-) and (+,)(+,-) with (,+)(-,+).

Two readings. Exactly two.

What the second reading costs, against how close the eye isA parallel drawing sits at the origin: the reversed reading is a cube, exactly, and nothing in the picture rules it out. A perspective drawing rules it out at a rate exactly inverse in the eye's distance — 0.39° at 128 m and 27.56° at 2.2 m — and never at all.010200.1000.2000.3000.4001 / distance from the eye to the box (per metre)worst angle between edges the box has parallel (°)parallel projection: 0.000°55° at the near endthe line through the origin is the inverse law
Fig. 2 The solid version, from its own essay: how the two readings of a drawn corner separate as the projection becomes more parallel, and how the ambiguity is complete at the limit.

And they are not the supplement of each other

The natural guess is that the phantom is 180°ϕ180° - \phi, or 360°ϕ360° - \phi: the fold read the other way, opened out or turned inside out.

Neither. Sweep the true dihedral from forty degrees to a hundred and sixty and the phantom traces a curve that touches neither of those, and by margins of several degrees at their closest.

The second reading is neither the supplement nor the reflexThe phantom against the truth, for a fold seen from 58° off the hinge's own plane. The straight line is where the two would be equal; the curve is what the drawing actually admits. At 40° the phantom is 50.4° and at 160° it is 125.2°, so the phantom is the shallower reading for deep folds and the deeper one for shallow ones, and the two cross at 66.1° — one dihedral that is its own phantom. Neither 180 − φ nor 360 − φ is anywhere on this curve, which is worth having because both are what a reader would guess. Move the ray and the crossing moves with it, which is what says it is a property of the drawing.501001505075100125150the dihedral the plate actually has (degrees)the other dihedral admitted (°)its own phantom at 68.2°seen from 59° off the hinge's planecrossing at 68.2°
Fig. 3 The phantom against the truth, for one viewing direction. The straight line is where the two would be equal; the curve is what the drawing actually admits, and it is not either of the two functions a reader would guess. Move the ray and the whole curve moves.

The reason the guesses are wrong is that they are answers to a different question. The supplement is the dihedral of the fold with one plate reflected in the hinge’s plane, which is an operation on the plate. What the drawing admits is the fold with one plate’s out-of-picture component reversed, which is an operation on the reading — and the two coincide only when the viewing direction is aligned with the fold’s own symmetry.

That distinction is easy to miss because the picture looks the same in both cases: two rays from a point, at some drawn angle. The drawn angle does not determine the dihedral at all, and the essay’s whole content is what does.

The phantom is shallower for a deep fold and deeper for a shallow one

Read the curve and it has a shape.

For a fold near a hundred and sixty degrees — nearly flat — the phantom is around a hundred and eighteen: much sharper. For a fold near fifty, the phantom is around fifty-six: slightly shallower. So the map compresses: it drags every fold toward a middle.

And the two cross. Somewhere between them is one dihedral that is its own phantom — at sixty-six degrees for the ray this figure uses — and there the ambiguity has no consequence, because both readings are the same plate.

One drawing, two plates: 66.0° and 66.0°Two plates hinged along one line at 66°, drawn orthographically. The drawn angle between the two plate edges is 60.14°, which is neither reading. The drawing fixes each edge's component in the picture and leaves its component along the ray free up to a sign, and an overall reflection identifies two of the four sign pairs — so there are exactly two plates consistent with these marks, at 66.000° and 66.049°. This is the Necker reversal moved from a solid's corner to a sheet's fold, and the second reading is not the supplement of the first: 180 − 66 is 114°, which is not on the list.one platethe otherthe hingedrawn at 60.1° · reads as 66.0° or 66.0°an orthographic drawing of a foldtwo readings, 0.0° apart
Fig. 4 The self-phantom, drawn. The two readings coincide, so this fold is the one dihedral a drawing from this direction is unambiguous about — and the direction is what puts it at sixty-six rather than anywhere else.

That crossing moves with the viewing direction. Change the ray and it lands somewhere else, which is what says it is a property of the drawing rather than of folds — and it is the reason the essay quotes it with the ray attached rather than as a constant.

The second reading is neither the supplement nor the reflexThe phantom against the truth, for a fold seen from 78° off the hinge's own plane. The straight line is where the two would be equal; the curve is what the drawing actually admits. At 40° the phantom is 53.8° and at 160° it is 153.1°, so the phantom is the shallower reading for deep folds and the deeper one for shallow ones, and the two cross at 124.8° — one dihedral that is its own phantom. Neither 180 − φ nor 360 − φ is anywhere on this curve, which is worth having because both are what a reader would guess. Move the ray and the crossing moves with it, which is what says it is a property of the drawing.501001505075100125150the dihedral the plate actually has (degrees)the other dihedral admitted (°)its own phantom at 124.8°seen from 78° off the hinge's planecrossing at 124.8°
Fig. 5 The same map from a different direction. The crossing has moved and the shape of the curve has changed with it, so neither the self-phantom nor the size of the ambiguity is a constant of folds.
One drawing, two plates: 150.0° and 118.3°Two plates hinged along one line at 150°, drawn orthographically. The drawn angle between the two plate edges is 147.67°, which is neither reading. The drawing fixes each edge's component in the picture and leaves its component along the ray free up to a sign, and an overall reflection identifies two of the four sign pairs — so there are exactly two plates consistent with these marks, at 150.000° and 118.269°. This is the Necker reversal moved from a solid's corner to a sheet's fold, and the second reading is not the supplement of the first: 180 − 150 is 30°, which is not on the list.one platethe otherthe hingedrawn at 147.7° · reads as 150.0° or 118.3°an orthographic drawing of a foldtwo readings, 31.7° apart
Fig. 6 A shallow fold, near flat. Its phantom is far away, so this is where the ambiguity costs most — a nearly flat plate can be read as one bent through a right angle.

Why the drawn angle is not either reading

There is a number on the paper that a reader will want to be one of the answers, and it is not.

The drawn angle between the two plate edges is what a protractor laid on the drawing measures. For a hundred-degree fold seen from a general direction it comes out at ninety-four — between the two readings and equal to neither.

The reason is that a projection foreshortens the two edges by different amounts. Each edge is drawn at LL times the sine of its own angle to the ray, and the two angles differ, so the drawn triangle is not similar to the true one. A protractor is measuring a third thing.

That is the same trap the true shape of a cut reports on a plane section: the area comes off the drawing with one number and the angles do not, because a foreshortening scales one direction and not the other. A fold is that finding on two half-planes instead of one polygon.

So a drawing of a fold carries three angles — the true dihedral, the phantom, and the one on the paper — and the third is the only one anybody can measure directly. It is worth saying plainly, because a reader who has been told the drawing is ambiguous will still reach for the protractor.

True length, point view, true shapeThree views of one face, differing only in the direction they are taken along. The first is chosen perpendicular to the marked edge, so that edge is at true length, 1.3928 m. The second is taken along that edge, so the edge is a point and the face is a line. The third is along the face's own normal, and the face is at true shape — 1.3232 m². Nothing is measured off the paper; each is the projection the chosen direction produces.true length1.3928 mpoint viewthe edge is one pointtrue shape1.3232 m²one face, three ray directionseach step is a choice of direction, not a construction on the paper
Fig. 7 The plane version of the same trap: a cut whose drawn angles are wrong by a computable amount and whose drawn area is wrong by a cosine.

The control, which is not the flat plate

Every claim on this site is paired with a case where it fails, and here the obvious candidate for that case is wrong.

The natural control is a flat plate — a dihedral of a hundred and eighty degrees, the two edges collinear and opposite. Surely a straight drawn line has one reading?

It does not. A straight line is also the drawing of a folded plate seen along the plane that bisects it, and the machinery duly returns two readings that differ by forty degrees. That is not a bug; it is a genuine degeneracy, and a control has to be a case where the ambiguity goes away rather than a case that looks unambiguous.

The case where it goes away is a plate edge lying in the picture plane, drawn at true length. Then the component along the ray is zero, and its two signs are the same number. One reading.

True length, point view, true shapeThree views of one face, differing only in the direction they are taken along. The first is chosen perpendicular to the marked edge, so that edge is at true length, 1.3928 m. The second is taken along that edge, so the edge is a point and the face is a line. The third is along the face's own normal, and the face is at true shape — 1.3232 m². Nothing is measured off the paper; each is the projection the chosen direction produces.true length1.3928 mpoint viewthe edge is one pointtrue shape1.3232 m²one face, three ray directionseach step is a choice of direction, not a construction on the paper
Fig. 8 The condition, from the auxiliary-view drill: an edge drawn at true length is an edge perpendicular to the ray, and it is the one case that carries no depth ambiguity because it has no depth in the picture at all.

So the control the check uses is a fold viewed so that one plate is edge-on to the ray, and it asserts the two readings agree to six decimal places. Finding that the flat plate was not the control is the kind of correction this site’s habit produces: the assertion was written, it failed, and the failure turned out to be a result rather than a mistake.

What the drawing does fix

It is worth being explicit about what survives, because “two readings” is easy to hear as “nothing is known”.

The drawn angle is fixed — it is on the paper — and it is neither reading.

The hinge’s direction in the picture is fixed.

And given the two plates’ lengths, the pair of admissible dihedrals is fixed: a finite set with two elements, not a family. That is a much stronger statement than the reversal makes about a general drawn corner, where Pohlke’s theorem says any three drawn segments from a point are the image of a cube’s edges — a one-parameter family of readings rather than two.

The difference is the known lengths. Pohlke’s freedom is exactly the freedom to choose the drawing’s scale and axes; fixing the plates’ actual sizes uses that freedom up, and what is left is the sign.

isometric: the drawn axes, and the cube they are a picture ofThe three vectors on the left are the whole input. The cube on the right, its edge of 1.0000 and the projection direction 0.0000° off the picture plane's normal all come out of them in closed form, and projecting that cube along that direction reproduces the drawn axes to 1e-16.what was drawnthe solid it depicts — reading 1 of 2xyzlooked at 0.00° off the normalcube edge 1.0000 of the drawn unitresidual 1e-16
Fig. 9 Pohlke, from its own essay: any three lines drawn from a point are the drawing of some cube. Knowing the lengths of the things being drawn is what collapses that family to a pair.

The dihedral, computed from the edges rather than from the normals

A small piece of machinery is worth pulling out because the obvious implementation of it is wrong in a way that passes most tests.

The dihedral between two half-planes sharing a hinge is the angle between the two plate edges measured perpendicular to the hinge. Not the angle between the edges themselves — an edge may have a component along the hinge, and that component belongs to neither plane’s inclination.

The other natural route is through the two planes’ normals: build n^a=x^×u^a\hat n_a = \hat x \times \hat u_a and n^b=x^×u^b\hat n_b = \hat x \times \hat u_b, take the angle between them, and take the supplement. That works and it carries a sign convention that has to be got right, and getting it wrong produces an answer that is correct for half the range and reflected for the other half — which looks like a plausible curve and is two functions glued together.

foldReadings takes the first route. It projects each edge perpendicular to the hinge, asserts that neither projection has collapsed to nothing, and takes the angle between what is left. The assertion is the part that matters: an edge drawn along the hinge has no perpendicular component and no dihedral to contribute, and a routine that returned an angle for it would be returning the arc-cosine of a zero over a zero.

That is the refusal the gate exercises, and it fires on a fold viewed along its own hinge — the one direction from which a fold draws as a single line and says nothing whatever.

A workshop reading of it

The practical form is short and is worth having, because a fold is a thing somebody makes.

A folded part on a drawing carries its bend angle as a number, never as something to be read off the drawn angle. That is universal practice and this is why: the drawn angle is not the bend angle, and even the pair of dihedrals the drawing admits needs the projection direction to be known before it can be worked out.

And a part’s bend direction — up or down, toward the reader or away — is marked with a symbol or a section rather than left to the drawing. That is the phantom being ruled out by an annotation.

Both conventions exist because a fold’s drawing is ambiguous, and neither of them says by how much. The map above says by how much: a hundred-degree fold reads as eighty-seven as well, which is thirteen degrees of ambiguity on a dimension that a bracket’s fit depends on.

One drawing, two plates: 90.0° and 80.5°Two plates hinged along one line at 90°, drawn orthographically. The drawn angle between the two plate edges is 84.04°, which is neither reading. The drawing fixes each edge's component in the picture and leaves its component along the ray free up to a sign, and an overall reflection identifies two of the four sign pairs — so there are exactly two plates consistent with these marks, at 90.000° and 80.487°. This is the Necker reversal moved from a solid's corner to a sheet's fold, and the second reading is not the supplement of the first: 180 − 90 is 90°, which is not on the list.one platethe otherthe hingedrawn at 84.0° · reads as 90.0° or 80.5°an orthographic drawing of a foldtwo readings, 9.5° apart
Fig. 10 A right-angle fold, which is the commonest thing a workshop makes. Its phantom is eighty degrees, so the drawing alone is consistent with a bracket ten degrees out of square.

The check that disagreed with its author

The control above is the second thing in this essay that came out of an assertion failing, and both are worth recording because the pattern is the site’s own.

assertADrawnFoldHasAPhantom was written with three parts. Every true dihedral has to be one of its own two readings — otherwise the reading machinery is wrong rather than the drawing ambiguous. The phantom has to differ from both the supplement and the reflex by a real margin. And a flat plate has to have one reading.

The third failed, and the reason turned out to be the finding above: a straight drawn line is also the drawing of a fold seen along its bisecting plane. The assertion was replaced by the edge-on control and the flat case was kept as a positive assertion in the other direction — that the two readings differ by more than a degree — so the degeneracy is on the record rather than quietly dropped.

That is the third time in two phases on this site that a check disagreeing with its author has produced the result rather than a repair. The habit that makes it work is writing the assertion before knowing the answer, which is uncomfortable and is the whole point.

One drawing, two plates: 45.0° and 53.4°Two plates hinged along one line at 45°, drawn orthographically. The drawn angle between the two plate edges is 40.27°, which is neither reading. The drawing fixes each edge's component in the picture and leaves its component along the ray free up to a sign, and an overall reflection identifies two of the four sign pairs — so there are exactly two plates consistent with these marks, at 45.000° and 53.421°. This is the Necker reversal moved from a solid's corner to a sheet's fold, and the second reading is not the supplement of the first: 180 − 45 is 135°, which is not on the list.one platethe otherthe hingedrawn at 40.3° · reads as 45.0° or 53.4°an orthographic drawing of a foldtwo readings, 8.4° apart
Fig. 11 The far end of the slider, at a sharply folded plate. Its phantom is the nearer of the two on the map’s whole range, which is the compression the curve shows read at one point.

Where this sits among the field’s ambiguities

The parallel field has now measured four different things a parallel drawing leaves free, and they are four different kinds of freedom.

The reversal leaves a binary choice about which corner is nearer, on a solid.

Pohlke leaves a continuum: any three drawn axes are some cube’s.

One oblique drawing leaves a one-parameter family of solids, sheared along the projection’s own kernel.

And a drawn fold leaves a pair, of which one is the plate and the other is a specific different plate whose dihedral is computable.

A dimensioned drawing is the solidEvery edge of the block runs along a world axis, and the drawn axes are scaled copies of those axes — so walking the edge graph from one corner gives every vertex back, to 1e-16 of a unit. The apex is joined by nothing axis-parallel: it slides 0.00 along the projection's kernel and its mark does not move by 0e+0 px. What closes a single parallel view is not a second view, it is the correspondence.plan: the apex has movedfree along the kernelisometricrecovered to 1e-16
Fig. 12 The third of the four: one drawn projection and the family of solids consistent with it. A fold’s pair is the discrete relative of the same phenomenon.

Putting them side by side is worth doing because the fold’s case is the one with the most structure. A binary choice is a choice; a continuum is a shrug; a pair whose second member is a computable other object is something a reader can go and look for.

What each extra parallel view buysThe metric upgrade has six unknowns and each view supplies three equations. Two views give six equations of rank five, so a one-parameter family of solids draws both pictures. Three give rank six and the family collapses to a point. What no count removes is the mirror image: at three views it still redraws every picture to 8e-16 px and is 100% of the object's own size away from it.2 viewsrank 51 free parameter3 viewsrank 6determined4 viewsrank 6determined5 viewsrank 6determinedsix unknowns in the upgrade, three equations per viewthe reflection is free at every count
Fig. 13 And the family a pair of parallel views leaves, from the same field. Two views collapse the reversal and leave a relief; one view of a fold leaves a phantom.

What a second view does

The obvious repair, and it works.

A second parallel view from a different direction fixes each plate edge’s component along the first ray, because that component is in the second view’s picture. So two views determine the fold — one reading, no phantom — which is the same statement as two parallel views collapsing the reversal and leaving only a relief.

What the second view does not fix is the relief: the whole arrangement can still be stretched along the common viewing direction, and a fold stretched that way has a different dihedral. So two views give the dihedral only if the two directions are known relative to each other, which on a drawing they are — the standard three views are perpendicular by construction, and that is what makes the convention work.

Three views, and two solids that draw themA stepped block with a hole on a 6-cell grid. The three views along the top are drawn by the 192-cell solid on the left and by the 64-cell solid on the right — every filled square in every one of the three views is filled by both. The views bound the solid and do not determine it.front view · 32 filledtop view · 36 filledside view · 36 filledthe largest solid with these views — 192 cellsand a solid with the same views — 64 cells6 × 6 × 6 cellsthe three views are identical; the solids differ by 128 cells
Fig. 14 The multiview method’s own limit, which the fold sits comfortably inside: three views leave some solids ambiguous, and a hinged pair of plates is not one of them.

What this does not settle

It does not treat a fold with plates of unknown length. Then the drawing admits a family rather than a pair, and the pair here is bought entirely by knowing how big the plates are.

It does not treat a curved fold — a plate bent through a radius rather than along a crease. That is the bent plate and its ambiguity is a different question, because a bend has a whole family of generators rather than one hinge.

And it does not say a reader ever mistakes one for the other in practice. Shading, hidden lines, an annotation and knowing what the part is for all remove the ambiguity long before geometry does — which is true and is a fact about drawings rather than about projection.

An ambiguity worth reporting is one whose second answer is a nameable object. “The drawing does not determine it” is a shrug; “the drawing is equally consistent with this other plate, whose dihedral is eighty-seven degrees” is something to check.

What the second reading costs, against how close the eye isA parallel drawing sits at the origin: the reversed reading is a cube, exactly, and nothing in the picture rules it out. A perspective drawing rules it out at a rate exactly inverse in the eye's distance — 0.39° at 128 m and 27.56° at 2.2 m — and never at all.010200.1000.2000.3000.4001 / distance from the eye to the box (per metre)worst angle between edges the box has parallel (°)parallel projection: 0.000°55° at the near endthe line through the origin is the inverse law
Fig. 15 The solid’s version of the same ambiguity at a longer distance, where the projection is nearly parallel and the two readings of a drawn corner are equally good. This essay is the sheet-metal relative of it.
The image of a circle in the xy plane, in 4 systemselevation and cavalier draw this plane isotropically — the circle stays a circle at 1.0000, so a length in it can be taken off the paper with a ruler whichever way it runs. The others draw it as an ellipse, and the ratio printed under each is the factor a ruler is wrong by between the best direction and the worst.elevation1.0000a circlecavalier1.0000a circleisometric0.57741 : 1.732military0.57741 : 1.732the xy plane's drawn ellipseratio of the ellipse's axes, sampled
Fig. 16 What the drawing does keep, from the field’s own table. The ambiguity is about depth alone; everything in the picture plane is exact and is what makes the pair of readings finite.

Shares its objects with

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

Named objects

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

DemonstrationDepth ambiguityDihedral angleDrawing systemForeshorteningFree parameterMultiviewOrthographicreconstruction ambiguityReversal ambiguityTrue scale