What survives

The polar with a straightedge

Two secants through a point cut a conic at four places; the complete quadrangle they make has two more diagonal points; the line through those is the polar. Not one length, angle or midpoint is used, so the whole construction survives the projection that made the picture — and three unrelated pairs of secants land on the same line to 4.3e-13, while moving the point moves it by fifteen orders of magnitude more.

Worth reading first: The diagonals find the middle · The circle whose centre moves.

There is a small family of constructions on this site that use no measurement at all. They draw lines through pairs of points and mark where lines cross, and nothing else. That restriction is not asceticism: it is the exact condition for a construction to survive a projection, and therefore the exact condition for it to be carried out on a photograph of a thing rather than on the thing.

The polar of a point with respect to a conic is the most useful member of that family, and this essay is about doing it with a ruler.

The polar of a point, with a straightedge onlyTwo secants through the point cut the conic at four places. The other two diagonal points of the quadrangle they make are joined, and that line is the polar — agreeing with the matrix product to 2.0e-13. No length, no angle, no midpoint: only joins and crossings, which is why the whole construction survives the projection that made this picture.the pointone point, one conicconstructed and computed agree to 2e-13
Fig. 1 Two secants through the point cut the conic at four places. Join those four crosswise, mark the two new crossings, and the line through them is the polar — agreeing with the matrix product to arithmetic noise. No length, no angle, no midpoint anywhere in it.

The construction

Take a conic and a point PP not on it.

Draw any two lines through PP that cut the conic. The first meets it at AA and BB; the second at CC and DD.

Those four points form a complete quadrangle. A complete quadrangle is four points and the six lines joining them in pairs; the six lines meet in three diagonal points, and one of them is PP itself, being ABCDAB \cap CD.

The other two diagonal points are ACBDAC \cap BD and ADBCAD \cap BC. Mark them.

The line through those two is the polar of PP.

That is all of it. Six lines drawn, three crossings marked, one line drawn through two of them. A child with a ruler can do it and it is exact.

Why it is worth having

The algebraic definition is shorter still: writing the conic as a symmetric matrix CC, the polar of PP is the line CPC\,P. One matrix product.

So why construct it?

Because the matrix product needs the conic’s coefficients in some coordinate system, and the construction needs nothing at all. Handed a photograph with a conic in it and a point marked, the construction gives the polar of that point in the picture — and because every step is an incidence, and incidences survive projection, that line is the image of the polar in the world.

Which means the construction transports a fact about the world through a picture whose camera is unknown, unrecorded and unrecoverable. That is the property the whole foundations field is built to collect.

Halving a receding rectangle two waysThe diagonals cross at the image of the rectangle's centre, 3e-14 px from it — the construction is exact at every camera because it uses only which lines meet where, and that is what a projection keeps. Halving the drawn side with a ruler instead lands 10.5 px from the image of the side's midpoint. The same diagonal continued lays out 3 more bays of the same 2.1 m, with nothing measured.the diagonals against a ruler, at 5.0 mthe diagonals — exactthe ruler — 10.5 px outcorrect from 26 cm, at 160 mm wideharmonic set -1.000000 · 3e-14 px
Fig. 2 The construction this one is a curved cousin of, and the reason both work. Four points in harmonic position, built with a straightedge from a complete quadrangle, and surviving the projection that made the picture — because a harmonic set is a cross-ratio of −1 and a cross-ratio is what a projection keeps.
Four points on a line, before and after a projectionLength and the ratio of lengths do not survive the projection; the cross-ratio does, agreeing to 0e+0 relative. Joined to a vertex off their line, the four points become four lines whose own cross-ratio is the same number — and two further transversals cut those lines in four points that carry it again, which is why any picture of the four rays gives the same answer.horizonABCDany vertexon the groundin the picturelength AB1.00011.3930ratio AB:CD0.56670.6837cross-ratio1.31681.3168correct from 26 cm, at 160 mm wide34° across
Fig. 3 The invariant underneath. Length goes, the ratio of lengths goes, the midpoint goes; the cross-ratio survives, in the points and in the pencil of lines through any vertex. A construction that uses only joins and crossings can only ever produce quantities of that kind.

Checking it, and checking that the check means something

The construction and the matrix product are two independent routes to one line, so they can be compared. Normalised so that the coefficient pair (a,b)(a,b) has unit length — a line being defined only up to scale and sign — they agree to about 4×10134\times10^{-13}.

That number on its own is worth very little. Two lines built from four points on one conic will tend to be near each other whatever the method, and a construction that quietly returned some fixed line would agree with itself perfectly.

So the test has a second half. The secants are varied. Three unrelated pairs of chords through the same point, three complete quadrangles with no vertices in common, three constructed lines — and all three land on the algebraic polar to the same tolerance.

Three different pairs of secants, one lineThree unrelated pairs of secants through one point, three complete quadrangles, three constructed lines. All three land on the algebraic polar to 4.0e-13, while moving the point 47 px moves that line by 1.2e+2 — so the agreement is about the construction rather than about a line that never moves.the pointthree pairs of secantsconstructed and computed agree to 4e-13
Fig. 4 Three pairs of secants through one point, three quadrangles, one line. The claim is that the answer does not depend on which chords were chosen, so a figure that used a single fixed pair would be showing that the construction closes once.

And a third half, which is the control. Move the point and the line has to move. Shifting PP by a few dozen pixels moves the polar by tens of pixels on the same normalised scale — fifteen orders of magnitude more than the disagreement between the two methods. Without that, a routine insensitive to its input would pass everything above.

That is the pattern every claim here is asked to have: the thing that should agree, the freedom it should be indifferent to, and the parameter it must not be indifferent to.

What the polar of a point is

The construction is exact before it is interpreted, but the interpretations are what make it useful, and there are four worth carrying.

It is the harmonic partner. Take any line through PP cutting the conic at XX and YY. It meets the polar at one further point QQ, and (X,Y;P,Q)(X, Y; P, Q) is harmonic — cross-ratio exactly 1-1. That holds for every line through PP, which is the strongest way to state what the polar is, and it makes the connection to the diagonal-point constructions exact rather than analogical.

It is the chord of contact. If PP is outside the conic, the two tangents from it touch at two points, and the polar is the line through them. So the construction hands over the tangents for free — draw the polar, mark where it cuts the curve, join those to PP.

The polar is the chord of contact, so it hands over the tangentsThe point is outside the conic, so its polar cuts the curve, and the two crossings are exactly where the tangents from the point touch. Both are found with a straightedge — the construction never measures anything — and they agree with the algebraic polar to 4.0e-13.the pointone point, one conicconstructed and computed agree to 4e-13
Fig. 5 The chord of contact. The point is outside the conic, the polar cuts the curve, and the two crossings are exactly where the tangents touch — obtained with the same six lines and no measurement.

It is a duality. The map “point to its polar” is a bijection between points and lines, and it reverses incidence: if PP is on the polar of QQ, then QQ is on the polar of PP. That single sentence is what makes conics the natural home of duality on this site, and it is what the essay on four lines and their cross-ratio is quietly using.

And it is a fixed structure. The map that sends every point to the harmonic conjugate of itself across the conic — the polarity — is an involution, and it is the fixed structure that distinguishes conic-based constructions from the homologies and elations the plane-map census sorts.

A homology: an axis, a centre, and one ratioEvery point moves along the line joining it to the centre, by the same ratio 2.4000; every point of the axis stays where it is. Three numbers, and the arrows are all that is left to draw.centrefaint dots: before · solid: afterhomologyratio 2.4000
Fig. 6 The census the polarity belongs beside. A homology has a line of fixed points and a centre; a polarity has neither, and pairs points with lines instead — a different kind of object, in the same room.

Where the construction stops

A construction is only as trustworthy as its refusals, and this one has three that are genuinely different in kind. Each is paired below with a case one step away that must still work, because a routine that refused everything would satisfy every refusal test ever written.

The centre. The polar of a conic’s centre is the line at infinity. That is not a failure of the construction — the quadrangle still builds, and the two diagonal points still exist — but the line through them is at infinity, which no normalisation can express as a finite line. The machinery here refuses rather than returning a very large number, and a point a thousandth of a unit off the centre has a perfectly good polar, which is asserted beside it.

Inside the conic. A point inside has a polar; it simply misses the curve, so there are no real tangents to hand over. The construction still works — the quadrangle needs the secants to cut, and every line through an interior point does — and what fails is the chord-of-contact reading. This is a refusal from the geometry, not a large residual, and it is the third time this site has had to record that distinction.

A secant that misses. From a point far outside the conic, most lines miss it entirely. Then there are no four points, no quadrangle, and nothing to construct. The failure is complete rather than degraded, which is the good kind: a solver that returned two complex intersections and carried on would produce a confident line from a construction that never happened.

The polar is the chord of contact, so it hands over the tangentsThe point is inside the conic. It still has a polar — the line is perfectly well defined and the construction still builds it, to 6.3e-13 — but the polar misses the curve, so there are no real tangents to hand over. That is a refusal rather than a large residual.the pointone point, one conicconstructed and computed agree to 6e-13
Fig. 7 The second refusal, drawn. The point is inside the conic, the polar is perfectly well defined and the straightedge still builds it, and the tangents do not exist. Reading the absence as a bug in the theorem is the mistake this figure exists to prevent.

The practical consequence for a reader working on a photograph is the third one: aim the secants at the curve, rather than drawing them in fixed directions. From an exterior point a randomly chosen direction usually misses, and aiming at a point known to be on the curve cannot.

The centre of a circle, from its photograph

The polarity is what settles a question this field has already asked twice, and the answer is worth having in one line.

The image of a circle’s centre is not the centre of the image. What is it? It is the pole of the horizon.

The circle’s centre is the pole of the plane’s line at infinity with respect to the circle. A projection carries poles to poles, so the image of the centre is the pole of the image of that line — which is the horizon. So: find the horizon, construct its pole with respect to the drawn conic, and that point is where the circle’s centre went.

And the pole of a line is constructed with the same straightedge, dually: take two points on the line, build each one’s polar, and the two polars cross at the pole.

A circle on the ground, and the two points that get called its centreThe image of the centre and the centre of the image ellipse are 14.6px apart — 4.0% of the ellipse's own width. The third mark is constructed from the drawn ellipse and the horizon alone, with no access to the circle: it lands 1e-14 px from the image of the centre and 14.61 px from the ellipse's own.centre of the ellipseimage of the centrepole of the horizon — 1e-14 px awaycorrect from 22 cm, at 160 mm widepole 1e-14 px from the truth
Fig. 8 The answer, drawn. The centre of the drawn ellipse and the image of the circle’s centre are two different points, and the second is the pole of the horizon with respect to the first’s own conic.
The centre offset against distance, for two circle sizesThe offset is largest for a near, large circle and never reaches zero until the circle's plane is parallel to the picture.02040603456distance from the eye to the circle (m)offset between the two centres (% of the ellipse's width)r = 0.50 mr = 1.00 mr = 1.80 mr = 2.60 mr = 3.60 mmeasured from fitted ellipses8.2% at 2.5 m
Fig. 9 How far apart they get. Not a small correction that careful drawing removes: the offset grows with the circle, because the near half is magnified more than the far half.

The identity that fell out of a tilted plane

There is a place on this site where a pole–polar relation turns up in a field with no conics drawn in it, and it is worth naming here because this essay is the machinery it was using.

Tilt a camera’s picture plane and two things move: the horizon drops from the principal point by ftanθf\tan\theta, and the vertical vanishing point arrives from infinity to f/tanθf/\tan\theta. Their product is f2f^2, at every tilt.

That is a polar relation. The horizon is the polar of the vertical direction’s vanishing point with respect to the absolute conic, and “the product of the two offsets is f2f^2” is what a polar relation looks like when both points are on the principal axis. It is also a one-line calibration from two things a straightedge finds in a photograph — which is this essay’s whole argument arriving somewhere it was not expected.

The picture plane tilted 18°Pointing the camera up tilts the picture plane with it, and three things happen at once: the verticals converge — 4.58° between the outer two — the horizon drops 277 px below the middle of the frame, and the vertical vanishing point arrives at 2628 px from the principal point. They are one fact: the product of those two offsets is f².correct from 20 cm, at 160 mm wideverticals converge 4.58° · horizon 277 px off centre
Fig. 10 The tilt that produces it. The horizon leaves the middle of the frame, the vertical vanishing point comes in from infinity, and the product of the two offsets is the focal length squared.
One conic, and the focal length falls out of itThe image of the absolute conic for a camera with square pixels is a circle of radius f about the principal point. Two vanishing points of perpendicular directions must be conjugate with respect to it, and solving that for f gives 1061.801 px — the same number the orthocentre construction gives, and 5.8e-13% from the focal length the camera was built with.horizonprincipal pointv_zorthocentre: 1061.8008 px · vᵀωu = 0: 1061.8008 pxconjugacy residual 0.0e+0 in focal-length unitscorrect from 25 cm, at 160 mm wide36° across
Fig. 11 And the conic the relation is taken with respect to. It is not drawn in any photograph, which is exactly why a construction that needs no measurement is the way to reach it.

The dual construction, for a line

Duality means every statement here has a partner, and the partner is the one that finds a pole from a line — which is what the circle-centre problem actually needs.

Given a line \ell, pick two points on it. Build each point’s polar with the quadrangle construction above. The two polars cross at one point, and that point is the pole of \ell.

The proof is the incidence reversal in one line: if XX is on \ell, then the pole of \ell is on the polar of XX; that is true for both chosen points, so the pole is on both polars, so it is their crossing.

Which makes the whole apparatus symmetric and equally cheap in either direction. Points to lines, lines to points, six drawn lines each time, and nothing measured.

The economy of incidence

It is worth being explicit about what class of statement this construction belongs to, because that class is small and everything in it is unusually durable.

A construction made only of joins (the line through two points) and meets (the point where two lines cross) is a projective construction. It commutes with every projectivity, so it can be done before or after a projection with the same result. There is no approximation involved: the result is not nearly the same, it is the same.

Everything else fails. A midpoint is not projective, so bisecting is out. An angle is not projective, so a perpendicular is out. A circle is not projective, so a compass is out. What survives is a ruler, and the surprising thing is how much can be done with one — the harmonic conjugate, the polar, the tangents, Desargues’ configuration, the repeated bay in a perspective pavement, the fourth point of a harmonic range.

That list is the reason the classical treatments spend so long on the complete quadrangle. It is not a curiosity: it is the only tool that works on a picture.

Two triangles in perspective from a pointCorresponding vertices lie on three lines through one centre. Pair off the corresponding SIDES instead and the three points where they meet are collinear — 5e-13 px from the line through them, at every configuration the slider reaches. Nothing was measured to make that happen, and nothing can be adjusted to improve it.three side intersections, collinear to 5e-13 pxcentrethree sides paired, three pointscollinear to 5e-13 px
Fig. 12 The theorem that makes incidence-only constructions feel inevitable. Two triangles in perspective from a point have their corresponding sides meeting on a line — proved, drawn, and closing exactly, with no measurement anywhere in it.
9 bays, built with a straightedgeOnly the first bay is measured. Every one after it is constructed: cross the diagonals to find the centre, run a line to the vanishing point to reach the midpoint of the far edge, then draw from the near corner through that midpoint to the receding line on the other side. After 9 bays the constructed corners are 1e-12 px from the corners the camera projects — which is arithmetic noise, not accumulated error, because the operation being iterated is a homology and not an approximation.horizoncorrect from 21 cm, at 160 mm wide9 bays · worst departure 1e-12 px
Fig. 13 And the same economy put to work in the construction field. Nine bays of a pavement laid out with a straightedge, landing where the camera would have projected them — because the operation being repeated is a projective one and not an approximation.

Why the quadrangle produces the polar

It is a short argument and it is worth having, because it shows that the construction is the harmonic property rather than a trick that happens to agree with it.

Let the two secants through PP meet the conic at A,BA, B and C,DC, D, and let E=ACBDE = AC \cap BD and F=ADBCF = AD \cap BC. Consider the line EFEF and where it meets the secant ABAB — call that point QQ.

The four points AA, BB, PP, QQ lie on one line, and EE, FF are two diagonal points of the quadrangle ACBDACBD with PP the third. The classical harmonic property of a complete quadrangle says exactly this: on any line through one diagonal point, the two vertices it passes through and the two points where the other diagonal meets it form a harmonic set. So (A,B;P,Q)=1(A, B; P, Q) = -1.

The same argument on the other secant gives (C,D;P,R)=1(C, D; P, R) = -1, where RR is where EFEF meets CDCD. So EFEF contains the harmonic conjugate of PP on both secants — and since the polar is defined as the locus of those conjugates, and two points determine a line, EFEF is the polar.

Two things follow that the drawing makes vivid. The construction is indifferent to which secants were used because the harmonic conjugate on each is determined by the conic and PP alone. And the whole argument is a statement about cross-ratios, which is why the projection that made the picture leaves it alone.

What to do with it

Three uses, in increasing order of how much they buy.

Find a tangent that is not drawn. The tangent to a photographed curve at a marked point is the polar of that point, and it is built with the straightedge — useful where the curve is drawn faintly or is partly hidden, since only five other marks on it are needed.

Find the centre of a photographed circle. Construct the horizon from any two families of parallels in its plane, then take its pole. The result is the image of the centre, which is the point a compass would have been placed at.

And find where the camera was. The polarity of a photographed circle relates the picture’s own geometry to the absolute conic, which is the object a focal length is read from — so a circle, a horizon and a ruler are between them a calibration. It takes two more rungs of this ladder to say exactly how, and this construction is the tool used at every one of them.

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.

centre of projectionComplete quadrangleConicCross ratioDualityHarmonic conjugateHorizonIncidencepole and polarProjective mapTangent