Surfaces that are not flat

The arcs the five-point construction actually draws

The taught five-point construction draws circular arcs between five vanishing points and instructs a draughtsman to graduate the radius evenly. Read that way, the arcs miss a straight line's true image by up to 3.75 pixels on a 300-pixel disc. Read at the stereographic scale instead, the same arcs are exact to 4.3e-13 pixels — the construction was always drawing one projection, and the taught scale was never it.

Worth reading first: The arcs a curvilinear drawing uses · Which rule a fisheye obeys, from straightness alone · Stereographic keeps every angle, and only stereographic.

The arcs a curvilinear drawing uses fitted a general conic to the image of a straight world line under six named picture surfaces and found exactly one surface — stereographic — returns something close enough to a circle to matter, to nine decimal places. That settled what the technique of drawing straight edges as arcs amounts to as a mapping. It did not test the specific taught recipe for producing those arcs by hand: five vanishing points, a straightedge and a compass, and no mention anywhere in the instruction of what scale the radius is supposed to carry.

Which rule a fisheye obeys, from straightness alone built a fit that takes marks, is told which sets came from straight edges, and returns which of the four candidate rules — equidistant, equal-area, stereographic, orthographic, set out in full elsewhere in this collection — straightens them. That fit does not need a photograph. It needs marks and a claim about straightness, and the five-point construction supplies both without ever having passed through a lens.

Put the two together and the taught construction turns out to be exact — not approximately, to the arithmetic floor — under one specific radial scale, and off by several pixels under the one draughtsmen are actually told to use. The construction was always drawing a real projection. The instruction that accompanies it never named which one.

That gap between what a technique does and what its own instruction says it does is worth taking seriously rather than treating as pedantry, because the arcs a curvilinear drawing uses already found the same shape of gap in the surrounding practice: curvilinear perspective has been taught, as a recipe for handling a wide field, for sixty years without the surface it amounts to ever being named. This essay narrows that finding from the technique in general to the single most common named construction inside it, and asks the sharper question a general conic fit cannot: not merely “is there a surface these arcs resemble,” but “does the specific instruction a student is given — mark five points, graduate the radius evenly — actually produce it.”

Read off an evenly graduated radius, the arcs miss by up to 2.1 px on a 168 px discThe five-point construction on its own disc: the forward direction at the centre, up, down, left and right on the rim, and five straight world lines drawn as circular arcs between their two vanishing points. The heavy curves are the arcs the construction draws; the light ones are where each line's image actually falls when the disc is read by the equidistant rule. They coincide exactly for the line whose plane holds the optical axis, which the construction draws as a diameter, and for the line at ninety degrees, whose image is the rim itself. Between the two the arc is wrong by up to 2.10 pixels, worst at about 40° of tilt. What is approximate is not the arc but the radial scale: an evenly graduated radius is not the scale the arcs belong to.five points · worst 2.10 px5 straight lines, drawn as arcs between their vanishing pointsworst 2.10 px at 40° of tilt
Fig. 1 The five-point construction on its own disc: the forward direction at the centre, up, down, left and right on the rim, and five straight world lines drawn as the circular arcs the construction actually produces between their vanishing points. Read with an evenly graduated radius — the customary assumption — the heavy arcs and the true image of each line coincide exactly on the two axis lines and depart by up to 2.10 pixels between them, worst at about 40° of tilt.

What the construction specifies, and what it leaves to a draughtsman

The recipe itself is short. Mark the horizon and a vertical through the centre; put a vanishing point for “straight ahead” at the centre of the disc, and vanishing points for up, down, left and right on the rim, ninety degrees from the centre in every direction. Any other straight direction in the scene gets a vanishing point somewhere on the disc, and the line it belongs to is drawn as the circular arc through that point and the two points already fixed for its own plane. Compass and straightedge suffice for every step.

What the recipe never specifies is the one thing a projection needs to be a projection: a rule assigning a radius on the disc to an angle off the forward direction. A draughtsman using an ordinary protractor or a scale ruled in equal divisions reads the disc as though radius were proportional to angle — which is the equidistant rule, chosen not because the construction asked for it but because it is the only scale an unmarked ruler can supply. That silent substitution is the entire subject of this essay: the construction fixes the arcs precisely, by a compass-and-straightedge procedure with no ambiguity in it, and leaves the scale to whatever happens to be lying on the drawing table.

This is a slightly different failure than the one measured for the technique in general. A general conic fit asks whether the arcs, as a set of curves with no radius attached at all, resemble a circle under some surface — a question with no scale in it to get wrong. Attaching numbers to the disc is a second, separate step, needed the moment anyone wants to read a distance, an angle, or a vanishing point off the finished drawing rather than merely admire its outline, and it is exactly the step the taught recipe is silent about.

Two readings of one drawing

The arcs drawn above do not change when the assumed scale changes; only the angle a given radius is taken to represent does. That makes it possible to ask, of the identical set of drawn arcs, how far each of two candidate readings departs from the line’s true image.

Exact on the axes, 3.75 px out at 40° — and exact everywhere on the other readingThe construction's departure from the true image of the same line, against how far the line's own plane is tilted from the one containing the optical axis, on a disc of 300 pixels. Read off an evenly graduated radius the departure is exactly zero at both ends and rises to 3.75 pixels in between — zero at nought because such a line images as a diameter and a diameter is what the construction draws, zero at ninety because that line images as the rim. The lower line is the same construction read as a stereographic picture, where the departure is the arithmetic floor at every tilt. One drawing, two readings, and the difference between them is a choice of radial scale rather than a defect in the method.01234020406080tilt of the line's own plane away from the optical axis (degrees)how far the drawn arc misses the true image, in pixelsread off an even radiusread stereographicallya 300 px disc, 90° at the rim3.75 px at 40° · floor at every tilt on the other reading
Fig. 2 The construction’s departure from the true image of one line, against how far that line’s own plane is tilted from the one containing the forward direction, on a disc of 300 pixels. Read off an evenly graduated radius the departure is exactly zero at both ends of the sweep and rises to 3.75 pixels in the middle — zero at nought because such a line images as a diameter, which is exactly what the construction draws, and zero at ninety because that line images as the rim itself, again exactly what is drawn. The lower curve is the identical arcs read as a stereographic picture instead, where the departure sits at the arithmetic floor at every tilt.

Both curves start and end at the same two points for the same reason: on the axis and at the rim, every candidate scale agrees, because a diameter and the rim itself are landmarks no radial rule can disagree about. Between those two points the evenly graduated reading pays a real and growing price — 3.75 pixels at its worst, on a disc where the earlier essay’s photographic fit could resolve a rule from marks two orders of magnitude smaller — while the stereographic reading pays nothing at any tilt. One drawn object, two ways of attaching numbers to it, and only one of those two ways is describing what the compass actually put on the page.

The asymmetry between the two curves is worth dwelling on, because it is easy to misread the figure as showing two comparably good approximations. It does not. One reading is exact and the other is not; there is no tilt anywhere on the sweep where the evenly graduated curve does better than the stereographic one, and the gap between them is monotone through most of the range rather than merely occasional. That is the signature of a wrong assumption rather than a noisy measurement — a genuinely approximate method would scatter around some middle ground, and this one instead tracks a smooth, predictable curve away from a zero that a different reading reaches everywhere.

The independent check: fitting the four rules blind

The conic fit two rungs below this one already said stereographic was the surface that makes sense of arcs-as-a-technique in general. The departure curve above says the specific five-point recipe’s arcs match it too, at the right scale. Neither of those is the identifiability fit this collection built for exactly this kind of question, so it is worth running that fit as a third, independent check.

The construction's arcs fit the stereographic rule to 4.3e-13 px and no other rule at allThe four fisheye rules fitted to the construction's own arcs, as though they were marks read off a photograph — the same plumb-line fit the fisheye essays use, given no scene knowledge but which marks came from lines that are straight. Stereographic bottoms out at 4.3e-13 pixels, which is the arithmetic floor, at a focal length of 150.00 — exactly half the disc's radius, which is the stereographic rule that puts ninety degrees on the rim, so the agreement uses up no free parameter. The nearest other rule is equidistant at 0.76 pixels. The reason is one line of geometry: a circle drawn through the images of two antipodal directions unprojects, under stereographic, to a circle through two antipodal points, and a plane through a point and its antipode holds the centre — so that circle is a great circle, which is exactly the direction set of a straight world line.equidistant0.76 pxgreat circle: 11.0 pxequal-area1.20 pxgreat circle: 10.8 pxstereographic4.3e-13 pxgreat circle: 3e-13 pxorthographic4.55 pxgreat circle: 2.8 pxstraightness residual of the construction's arcs, on a log scale5 arcs on a 300 px disc, one focal length between themstereographic at f = 150.00 = R/2
Fig. 3 The four candidate fisheye rules fitted to the construction’s own arcs, treated as marks read off a photograph with no scene knowledge given — the identical plumb-line fit run on lenses and on the schematic eye elsewhere in this collection. Stereographic reaches 4.3 × 10⁻¹³ pixels, the arithmetic floor, at a fitted focal length of 150.00 — exactly half the disc’s own radius, which is the scale that puts ninety degrees on the rim and so costs the fit no free parameter at all. The nearest other candidate, equidistant, bottoms out at 0.76 pixels and does not approach the floor at any focal length.

A fit reaching the floor at exactly R/2 is not a coincidence dressed up as a measurement; it is the fit discovering, with no scene and no camera given to it, the same scale the departure curve found by direct comparison against a known line. Three separate routes — a general conic fit two rungs below, a direct comparison against a known true image, and a blind four-way identification — now agree on the same answer, which is the standard this site holds a claim to before calling it settled rather than merely observed once.

The reason is one line of geometry rather than a numerical accident. Two of the construction’s five vanishing points — up and down, or left and right — sit at opposite ends of a diameter of the disc, which is what a pair of perpendicular directions gives under any azimuthal scale. Under the stereographic rule specifically, two such antipodal points on the disc unproject to two antipodal points on the sphere of directions, and a plane through a point and its antipode always contains the sphere’s centre — so the circle that plane cuts is a great circle, and a great circle is exactly the set of directions a straight world line occupies. The construction’s arcs are great-circle images because two of the five points it is built from are antipodal, and stereographic is the one rule under which that antipodal relationship survives onto the page as a diameter.

That “antipodal points stay antipodal” property is not a fact special to this one construction; it belongs to stereographic projection generally, which is the same property stereographic keeps every angle already isolates from the other side, as the rule that preserves shape locally everywhere on the sphere rather than only along one favoured family of lines. What is specific to the five-point construction is only that a draughtsman’s own choice of layout — vanishing points for up, down, left and right, spaced a quarter-turn apart around the centre — happens to hand the construction two genuinely antipodal pairs for free, without anyone drawing the construction needing to know that antipodal points are the object being exploited.

The control: take three points away and there is nothing left to misread

If the trouble above is specifically about curvature — about a disc trying to carry a sphere’s worth of directions — then removing the curvature from the question ought to remove the trouble along with it. The construction offers exactly that reduction on its own terms: run it with only the centre point and one pair of opposite vanishing points, and there is no longer a third direction for an arc to bend toward.

Two vanishing points and straight lines: the marks are collinear to 1.1e-13 pxThe control, and it is the five-point construction with three of its points taken away. With only two vanishing points there is nothing for an arc to bend between, the construction draws straight lines, and on a flat picture plane that is exactly right: every mark along each world direction lies on the line joining its first mark to its vanishing point, to 1.1e-13 pixels over 34 marks. So the machinery that reports pixels of departure for the five-point construction reports the arithmetic floor when there is nothing to report, which is what makes the earlier numbers measurements rather than a property of the ruler.vanishing point 2correct from 11 cm, at 160 mm widecollinear to 1.1e-13 px
Fig. 4 The construction stripped to two vanishing points, at a field of view of 72°. With nothing for an arc to bend between, every mark along a world direction lies on the straight line joining its nearest mark to its own vanishing point, to 1.1 × 10⁻¹³ pixels over 34 marks — the arithmetic floor, on an ordinary flat picture plane correct from 11 centimetres at 160 millimetres wide.

This is the control the whole essay needs, and it is worth reading as one. The five-point construction’s departure figures report a real, non-zero number precisely because there is a rule to get right and a rule the customary reading gets wrong. Take away the third vanishing point and the machinery that reported pixels of departure reports the floor instead — not because the construction improved, but because there is nothing left in a two-point drawing for a wrong scale to mismeasure. A flat plane has one honest reading of itself, and ordinary linear perspective is the special case where the disagreement this essay measures has nowhere to live.

No surface keeps everything is the reason a flat plane gets that one honest reading for free: it is the unique surface among the ones this collection measures that draws every straight world line as a straight line, so a flat two-point drawing needs no radial rule at all to be read correctly — a straightedge laid between two marks already is the correct instrument. The moment a third vanishing point is added and an arc has to be struck between it and its neighbours, that free ride ends, because now there is a curve rather than a line, and a curve has to be read at some scale for its shape to mean anything angular at all.

Why the customary reading is wrong by exactly this much

The departure and stereo figures both report how much the evenly graduated reading misses by. What sets the size of that miss is the same fact which rule a fisheye obeys already quantified for photographs: the four candidate rules for turning an angle into a radius agree closely near the centre of a field and separate substantially toward the edge.

Four rules that agree to first order and part by 54.0% at 45°The image radius each fisheye rule gives, against the angle off the optical axis, with every curve divided by its own value at ninety degrees so that the four are compared on their shape rather than on a choice of focal length. All four are the same straight line near the middle of the picture — each is fθ plus a cubic — and the cubic coefficients are equidistant 0.000, equal-area -0.042, stereographic 0.083, orthographic -0.167. That is the entire difference between them, and it is why identifying the rule from a picture is a question about the periphery. The flat plane is drawn as the control at the far end: it is not a fisheye rule at all and it is unbounded at ninety degrees.00.50011.500255075100angle off the optical axis (degrees)image radius, against the radius the same lens gives at 90°equidistantequal-areastereographicorthographicflat planeeach curve divided by its own radius at 90°54.0% apart at 45°
Fig. 5 The four candidate rules’ own radius, against angle off axis, each divided by its value at ninety degrees. Equidistant — the rule an unmarked ruler silently assumes — and stereographic — the rule the construction’s arcs actually obey — part by 54.0 per cent at 45° off axis, out of cubic coefficients of 0.000 and 0.083 respectively.

Reading a stereographic drawing on an equidistant scale is exactly the mismatch that 54 per cent divergence describes, applied to a construction rather than to a lens. Near the centre of the disc the two scales barely differ, which is why the axis lines in every figure above come out exact regardless of which reading is used; toward the rim they diverge substantially, which is why the departure curve’s worst point sits at an intermediate tilt rather than at either end. The five-point construction is usually recommended precisely for fields wide enough that this divergence is not small, which makes the mismatch a property of exactly the use case the technique is chosen for rather than an edge case around it.

The account of why the two rules diverge as a cubic in the angle off axis applies here without modification, because it is a fact about the pair of rules and not about whether a lens or a compass produced the picture. Near the disc’s centre both rules agree to first order, for the same reason every rule in that family does; the cubic correction that separates them is small there and grows toward the rim, so a mismatch invisible on the axis line becomes, at forty degrees of tilt, several pixels on a disc of a few hundred — the exact size this essay’s departure figure reports.

How much is at stake at the field this technique is sold for

The five-point construction earns its place in a draughtsman’s toolkit at fields ordinary linear perspective cannot reach at all — well past a hemisphere, where a flat plane’s picture would need to run to infinity. It is worth seeing what the scale confusion costs at a field in that range rather than only at the 90° used above.

Equal-area against equidistant: the same hall, 8.9 px apart at worst on a 168 px discTwo rules drawing one room from one place, superposed, both scaled so that 200° of the world exactly fills the disc. Nothing about the scene, the station point or the field differs; only the rule does. The two agree exactly at the centre and by construction at the rim, and the greatest disagreement between them is 8.9 pixels, in the middle band of the picture where neither constraint holds. That is what has to be measured through a marking error before anybody can say which rule took a photograph.equal-areaequidistant200° across, both rules at the same disc radius8.9 px apart at worst
Fig. 6 Two rules — equal-area and equidistant — drawing one room from one station, superposed on a disc scaled so that 200° of the world fills the frame. The two curves agree exactly at the centre and by construction at the rim; the greatest disagreement between them anywhere is 8.9 pixels on a 168-pixel disc.

Equidistant and equal-area — the pairing behind a mirror ball’s own picture — are not the pair this essay’s own construction confuses, which is equidistant against stereographic, but the figure is the right instrument for the general point, because it is the same machinery run at a field past a hemisphere rather than at 90°. Whatever gap two candidate rules carry at a given field, that gap only grows as the field opens further, which is exactly the direction the five-point construction is pushed toward in practice. A technique recommended for its very wide reach is a technique whose scale-reading error is recommended right along with it, growing rather than shrinking with the field that makes the technique worth using at all.

The lines every azimuthal surface agrees about

One more question is worth closing off before the essay’s limits: why do the two axis lines come out exact under every scale in every figure above, when nothing else does? The lines a surface leaves alone answers it for picture surfaces generally, and the same answer explains the construction’s two exact directions without needing a separate argument.

The lines each surface leaves aloneA curved picture surface does not bend everything. Each panel draws the family of world lines the surface images as straight lines: two-dimensional for the plane, and a one-parameter family for every other surface here — running through the picture's centre on an azimuthal surface, and parallel on a cylindrical one.planeevery linestereographicone parameter · concurrentthey meet to 1e-12equidistantone parameter · concurrentthey meet to 2e-62 of 3 keep a curvethe signature has three values, not eight
Fig. 7 Borrowed from the essay that measures it: the family of world lines each of three picture surfaces images as a straight line. The flat plane keeps every line straight, two-dimensionally. Stereographic and equidistant each keep only a one-parameter family — the lines running through the picture’s own centre — meeting there to within 1e-12 and 2e-6 respectively, of the four candidate rules used throughout this essay only two are drawn here, but the same fact holds for all: every azimuthal rule agrees on lines through the axis and disagrees everywhere else.

A line whose plane holds the optical axis is exactly the family every azimuthal rule — equidistant, equal-area, stereographic, orthographic alike — images as a straight line through the centre, because every one of those rules is built from the angle off the axis alone and such a line’s image inherits the world line’s own straightness by symmetry. The five-point construction’s up-down and left-right diameters are drawn as straight lines precisely because they belong to that family, and every candidate scale draws them correctly for the same reason every candidate rule agrees at the centre of the laws figure above: the disagreement between rules lives entirely off that one special family, which is exactly where the departure curve’s zeros sit.

What this does not settle

The measurement above is about where a set of arcs, already drawn, actually sit relative to a straight line’s true image. It says nothing about several things a full account of the technique would need.

It says nothing about whether a wide-field picture built this way looks more natural to a viewer than the same field forced onto a flat plane, which is the usual argument made in its favour and is a claim about perception this collection has no machinery for — the same limit the eye is a picture surface too states for a retina rather than for a drawing. It says nothing about a real hand-drawn construction’s compass and measurement error, which would sit on top of the exact-arcs case measured here rather than replacing it: a draughtsman’s actual arc, struck slightly off centre or read against a slightly warped sheet, adds its own residual to whichever of the two curves above it is closer to, and nothing in this essay’s arithmetic bounds that separate source of error.

And it says nothing about constructions built from a different number of named points — seven-point or nine-point variants exist in the drafting literature — which would need their own fit rather than inheriting this one, because the antipodal-pair argument above is specific to vanishing points that sit at opposite ends of a diameter, and a construction with an odd arrangement of points need not have any such pair at all. A construction without an antipodal pair anywhere in its layout has no guarantee of landing on stereographic, or on any other single named rule, and the honest answer for one would need the same three-way check run again rather than assumed from this one’s result.

One method, a third subject

The fit this essay leans on has now been run on a lens, on a schematic eye, and on a draughtsman’s construction that never passed light through anything. In every case the method is the same: take marks, accept nothing about their origin except which sets came from something straight, and ask which of four named rules straightens them. The eye is a picture surface too found the eye’s own geometry sitting near the equal-area rule, by coincidence of one animal’s proportions rather than by design. This essay finds the five-point construction sitting exactly on the stereographic rule, by a fact of its own geometry — two antipodal vanishing points — that holds regardless of what a draughtsman intends. Between the three, the fit has now told the difference between an approximate biological accident and an exact geometric one, which is a distinction no single figure of either kind could have shown on its own.

That distinction matters beyond this one construction, because taught geometry is full of instructions that specify a procedure and stay silent about what the procedure amounts to. A recipe that produces a correct answer for reasons nobody wrote into the recipe is not a lucky recipe; it is a piece of exact geometry wearing the clothes of a rule of thumb, and the fit this collection built for lenses is what let that geometry be read off a page that was never a photograph at all.

What links here

Computed from the collection, not written here: the essays that point at this one.

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.

Circle preservingConformalConic fitDrawing systemEquidistant projectionIdentifiabilityResidualStereographic projectionStraightedge constructionVanishing point