What each projection optimises

The average of two projections

The Winkel tripel is literally the arithmetic mean of two other projections, and this site's implementation of it agrees with that mean to the last bit. Averaging beats both ingredients by 26 per cent — and it preserves conformality exactly, destroys equal-area completely, and can turn eighteen per cent of the world inside out without either distortion measure saying so.

Most projections are built. A surface is chosen, a condition is imposed, an equation is solved, and what comes out has a construction anybody can follow.

A few of the most printed maps of the last century were not built that way at all. They were averaged: two existing projections, evaluated at the same point, and the two answers added together and halved.

Every mixture of Equirectangular at 50.46° and Aitoff. Airy's criterion over the whole sphere, for every weighted average of the Winkel tripel's own pair. Each mixture is normalised to its own best constant scale first, so the comparison is about shape rather than size. The curve has its minimum at w = 0.45, where the criterion is 0.3037 against 0.4114 and 0.4290 at the two ends. That is a projection nobody constructed beating both projections somebody did, by 26 per cent.
Fig. 1 Airy’s criterion over the whole sphere for every weighted average of the equirectangular projection at 50.46° and the Aitoff. Each mixture is normalised to its own best constant scale before scoring, so the comparison is of shape rather than size. The curve has an interior minimum: a projection nobody constructed beats both projections somebody did, by 26 per cent.

The Winkel tripel is an average, and the word is not loose

Oswald Winkel’s projection of 1921 is defined as the arithmetic mean of the equirectangular projection with standard parallel φ1=arccos(2/π)\varphi_1 = \arccos(2/\pi) and the Aitoff projection. The name says so: tripel is German for a triple, and refers to the three distortions the mean was meant to balance rather than to three ingredients.

The site’s own implementation is a transcribed formula that does not look like an average at all — an auxiliary angle, a cardinal sine, two terms over two. Asking whether it is the average is therefore a real question with a possible answer of no.

It is the average, to the last bit a double carries. Sampled every five degrees over the whole sphere, the largest discrepancy between the library’s Winkel tripel and the arithmetic mean of the library’s other two projections is exactly zero.

That is worth having as a check rather than as a remark. The blending machinery was written for this essay and the target was written long before it by somebody transcribing a formula, so agreement means neither is wrong.

What the mixture buys

The two ingredients score 0.4114 and 0.4290 on Airy’s criterion over the sphere. Every mixture between them scores better than both, and the best — at a weight of 0.45 rather than 0.5 — scores 0.3037.

That is a 26 per cent improvement over the better ingredient, obtained by an operation with no geometry in it whatsoever. It is the strongest available argument for compromise projections as a category, and it is the argument that category is almost never given: the usual defence is that a compromise “balances” the distortions, which is a description of the intent rather than a measurement of the result.

Winkel’s own half-and-half scores 0.3061, which is 0.8 per cent worse than the best mixture on this criterion. That is not a criticism of Winkel. It is a statement about the criterion: Airy’s is one weighting of one pair of quantities, and Winkel was balancing three. A projection built to minimise something else lands near the optimum of Airy’s without being at it, which is the ordinary situation and is what every projection minimises something is about.

Averaging does not always help, and the machinery says which

The interior minimum above is not a law. Mixing two equal-area projections — Mollweide and the sinusoidal — produces a curve with no interior minimum at all: the best mixture is pure Mollweide, at a weight of zero, and every step towards the sinusoidal makes the criterion worse.

Every mixture of Mollweide and Sinusoidal. Airy's criterion over the whole sphere, for every weighted average of two equal-area projections. Each mixture is normalised to its own best constant scale first, so the comparison is about shape rather than size. The curve has its minimum at w = 0.00, where the criterion is 0.4357 against 0.4357 and 0.5566 at the two ends. The minimum is at an end point, so mixing this pair gains nothing: the curve runs monotonically from the better ingredient to the worse, and the honest answer is to use the better one.
Fig. 2 The same sweep between two equal-area projections. The minimum is at an end point, so mixing this pair gains nothing and the honest answer is to use the better ingredient. The claim a caption makes about where the optimum lies is a parameter of this figure, and a caption that said “interior” over this pair would fail the build rather than print a sentence the picture contradicts.

So whether an average is worth taking is a question about the particular pair, and the only way to find out is to sweep it. That is a small piece of engineering with a large consequence for how the family of compromise projections should be read: it is not a technique that reliably improves things, it is a one-parameter search that sometimes has an interior answer.

Over a region rather than the world

The world is the hardest case and the one compromise projections were invented for, but the operation is not restricted to it, and over a region the numbers change character.

Every mixture of Mercator and Albers equal-area conic. Airy's criterion over europe, for every weighted average of a conformal cylindrical and an equal-area conic. Each mixture is normalised to its own best constant scale first, so the comparison is about shape rather than size. The curve has its minimum at w = 0.95, where the criterion is 0.0573 against 0.2570 and 0.0582 at the two ends. That is a projection nobody constructed beating both projections somebody did, by 1 per cent.
Fig. 3 Mercator and the Albers equal-area conic, mixed over Europe. Mercator alone scores 0.2570 on Airy’s criterion over the region and Albers 0.0582 — a factor of four apart, so this is not a contest between comparable ingredients. The optimum is nonetheless a mixture, at a weight of 0.95, and it scores 0.0573. Averaging in five per cent of a projection four times worse makes the result better.

That last sentence is the finding, and it is not an artefact of the criterion. A projection’s distortion has a pattern, and a small admixture of a projection whose pattern is oriented differently can cancel part of it — the same mechanism that makes fitting the aspect to the region worth a factor of 183, arriving through a different parameter.

The gain here is 0.8 per cent, which is small and is not the point. The point is that the sign is positive: the best member of the family is not the better ingredient, even when the ingredients are four times apart in quality.

Conformality survives averaging, and this was a surprise

The obvious expectation is that averaging destroys exact properties. Mix two projections that preserve angles and the result preserves nothing; mix two that preserve areas and the same.

Half of that is right and half of it is not, and the half that is not is the more interesting.

Every mixture of two conformal projections is conformal. Measured across three pairs and three weights each — Mercator with the stereographic, Mercator with the Lambert conformal conic, the stereographic with the conic — the largest angular deformation anywhere is 2.0×1062.0\times10^{-6} degrees, which is the noise floor of the differentiation and is fifty times below the tolerance measuring instead of naming sets for the property.

The reason is one line once the right words are used. A conformal projection of the sphere is a holomorphic function of the isometric coordinate — that is what conformality is, once the sphere is given its complex structure — and holomorphic functions form a vector space. Any weighted sum of them is holomorphic, hence conformal.

No mixture of two equal-area projections is equal-area. The condition there is that a determinant equals one, which is quadratic, and quadratic conditions are not preserved by averaging at all: the worst areal error across the same kind of sweep is 0.162, which is sixteen per cent and four orders of magnitude above the tolerance.

What that implies about compromise projections as a class

If mixing conformal maps can only ever produce another conformal map, then no mixture of conformal projections can be a compromise — a conformal map of the whole sphere has unbounded areal error, and no amount of averaging escapes it.

So a compromise projection has to include an ingredient that is not conformal. Winkel’s does: the equirectangular projection preserves nothing and the Aitoff is equal-area in neither of its coordinates. Neither ingredient is exact about anything, which is exactly the freedom the mixture needs.

That is a structural fact about the whole class, obtained from an algebraic property of one of the two conditions, and it is not in any account of compromise projections this site has found.

The failure neither distortion measure reports

There is a defect averaging can produce that has nothing to do with either exact property, and no quantity this site has defined so far can see it.

Where the mixture turns the ground inside out. The graticule of a half-and-half average of one projection, pointed two ways, with every cell whose Jacobian determinant has the opposite sign to the rest shaded. Inside the shading the map is a mirror image of the ground: east runs west and a country is printed reversed. 18.0 per cent of the sampled sphere is affected. Neither distortion measure this site computes reports it, because the areal factor is |det J| and the angular deformation is built from square roots, and both throw the sign away.
Fig. 4 The graticule of a half-and-half average of the Lambert azimuthal equal-area projection centred at 0° and the same projection centred at 90° east — the most innocuous mixture anybody could write down, being one projection pointed two ways. The shaded cells are where the Jacobian determinant has changed sign: the map has turned the ground inside out there, so east runs west and a country is printed as its own mirror image. It is 18 per cent of the sampled sphere.

The areal scale factor is detJ|\det J| and the two principal scales are square roots. Both throw the sign of the determinant away, so a folded region measures as an ordinary one. The mildest folded point on this map reports 4.98 degrees of angular deformation and an areal factor of 0.517 — numbers that would not raise an eyebrow anywhere on a compromise map.

Only near the fold line, where the determinant passes through zero and the areal factor runs away, does anything conspicuous happen. Away from it the defect is silent, and a projection library that reported the two usual quantities and nothing else would publish this map with a clean bill of health.

Why the fold happens, and when it does not

A mixture folds when the two ingredients’ derivatives point in sufficiently different directions. Two conformal maps cannot: their derivatives are complex numbers, the mixture’s derivative is the same weighted sum, and a sum of complex numbers is zero only if they oppose exactly — which is a curve in the plane, not a region.

Two azimuthal maps centred 90° apart do, because at points between the two centres one map is pulling east and the other north. Mixing them at any weight produces a region where the combined derivative has passed through zero and out the other side.

That gives a rule with no arithmetic in it: mixing two projections of the same aspect is safe and mixing two different aspects is not, and the site’s own aspect machinery makes the second easy to write by accident. Fitting the aspect to the region shows how much an aspect is worth; this shows what averaging across one costs.

Where the mixture turns the ground inside out. The graticule of a half-and-half average of the Winkel tripel's own pair, with every cell whose Jacobian determinant has the opposite sign to the rest shaded. Inside the shading the map is a mirror image of the ground: east runs west and a country is printed reversed. 0.0 per cent of the sampled sphere is affected. Neither distortion measure this site computes reports it, because the areal factor is |det J| and the angular deformation is built from square roots, and both throw the sign away.
Fig. 5 The same measurement on the Winkel tripel’s own pair. Not one cell is shaded: the two ingredients share an aspect, so their derivatives never oppose each other and the mixture cannot turn over. The same is true of any two conformal projections, for a stronger reason — the derivative of a holomorphic function is a complex number, and a weighted sum of two of them cannot reverse orientation without passing through zero on a curve rather than over a region — which is measured in the gate rather than drawn here.

What a mixture is, as a projection

It is worth being clear that a blend is a projection in the full sense this site uses. It is a map from the sphere to the plane; it has a Jacobian; every quantity here — the two principal scales, the areal factor, the angular deformation, the regional criteria — is defined on it and is computed the same way as for any library member.

What it does not have is a construction. There is no surface it was rolled from, no condition it solves, no viewpoint it represents. That is precisely why the question “is the average of two good maps a good map” cannot be answered by reasoning about the ingredients and has to be measured.

4 projections of the same sphere. The same graticule under Equirectangular, Winkel tripel, Robinson, Mollweide. Every one of them is a faithful drawing of the same object and no two agree, because each has chosen a different thing to preserve.
Fig. 6 Four world maps for comparison: the equirectangular projection, which is one of Winkel’s two ingredients; the Winkel tripel itself; Robinson’s, which is defined by a table of numbers somebody adjusted by eye; and Mollweide, which is exactly equal-area. Two of the four have a construction and two do not, and the two that do not are the two most likely to be found on a wall.

The rest of the class, and what it is not

Averaging is not the only way to make a projection without a construction. Robinson’s is a table of numbers adjusted until the result looked right, which is a different thing again and is where the indicatrix is a limit finds a projection whose derivative jumps at every table entry.

The distinction worth drawing is about what can be said afterwards. A blend inherits the differentiability of its ingredients, so every quantity this site computes about it is as well behaved as the ingredients’ own. A table with linear interpolation does not, and one of the site’s standing measurements — how large a circle Tissot’s ellipse describes — has no answer at all at a table entry on Robinson.

So the two ways of making a projection without solving a condition are not equivalent. One of them is arithmetic on smooth functions and the other is a lookup, and only the first leaves the machinery intact.

Where the mixture lands in the audit

Every projection this site holds is measured for angular deformation and areal error and plotted on one chart, and a blend can be measured the same way. The result is where a reader would expect a compromise to be and is worth seeing plotted rather than described: nowhere near either axis.

Every projection in the library, measured against both properties. Maximum angular deformation across the bottom, maximum areal error up the side, both on logarithmic scales and both measured over several hundred sample points rather than taken from the projection's description. Conformal projections lie on the left edge, equal-area ones along the bottom, and the corner where both vanish is empty because a projection there would be an isometry of the sphere onto the plane. All 26 are plotted; the five named here are Winkel tripel, Robinson, Mercator, Mollweide, Equirectangular.
Fig. 7 The site’s founding measurement, with the two averaged projections named on it. The empty corner near the origin is the claim that matters — nothing is close to both axes, and the trade-off forbids it. The Winkel tripel sits well out along both, which is what a compromise is: it has given up being exact about anything in exchange for being bad at nothing.

A compromise projection is therefore not a projection that is nearly conformal and nearly equal-area. It is one that is neither, deliberately, by an amount chosen so that the worse of the two failures is as small as possible. That reading is available from the chart’s geometry and is obscured by the word “compromise”, which suggests a middle rather than a minimax.

What the field says here

Which projection is best argues that the question is incomplete without a purpose. This essay adds that it is also incomplete without a set to choose from, and the set is larger than the library.

Between any two projections lies a one-parameter family, and its best member is usually neither end. A catalogue of named projections is a discrete sample of a continuous space, and the sampling is historical rather than mathematical: it contains the ones somebody published.

The measurement to make, given a purpose and a region, is therefore not “which of these twenty-one” but “which point in the space these twenty-one span”. That is a larger optimisation and this essay only opens it: two ingredients, one weight, one criterion.

The one thing an average cannot be asked for

An average has no exact property and therefore cannot answer a question that needs one. That sounds obvious and is routinely ignored, because a compromise projection is pleasant to look at and its failures are nowhere large.

The concrete cases are worth naming. A thematic map whose shading is per unit area needs the areas right, and a projection 30 per cent out in area over the region shades a lie; that is the projection that shows true size and the requirement is exact rather than approximate. A chart on which a bearing is plotted with a protractor needs angles preserved at the point of plotting, and a compromise’s angular deformation of 60 degrees in the corners is not a small residual. And a grid a survey computes in needs a scale factor with a closed form, which an average of two projections has only in the sense that it has a Jacobian.

So the class is exactly what its name says and no more: general-purpose maps, for readers who will not measure anything off them. The measurement in this essay says how good the best such map can be, and the answer — 26 per cent better than either ingredient — is the case for the class rather than against it.

What a mixture costs at the moment it is inverted

There is one practical price the audit does not report, and it falls on a use every map has: going from the page back to the ground.

A named projection usually has a closed-form inverse, and where it does not — the transverse Mercator’s series, the polyconic — the inverse is a known, published, tested piece of arithmetic. A mixture of two projections has neither. The forward map is a weighted sum of two formulas and is trivial; the inverse of a sum of two functions is not a sum of two inverses, and there is no reason for it to have a closed form at all.

So an averaged projection is inverted numerically, by a Newton iteration on the forward map, one point at a time. That is affordable and it is not free: a few evaluations of both parent projections and their derivatives per point, against one evaluation for a named projection with a formula. Where it bites is the places an inverse is used in bulk — georeferencing a scanned sheet, converting a screen click, warping a raster back, which is a per-pixel inverse.

And the iteration fails exactly where the essay’s fold is. A Newton step divides by the Jacobian, and the fold is the locus where the Jacobian’s determinant passes through zero. Approaching it, the iteration becomes ill-conditioned; at it, the inverse is undefined; beyond it, there are two ground points for one page point and the iteration converges to whichever the starting guess was nearer. That is not a numerical inconvenience — it is the fold reported in the units a user meets it in.

So the fold has a second consequence beyond the one already measured. It makes the map non-injective, which the distortion measures do not report, and it makes the map non-invertible in the concrete sense that the code returns an answer and the answer depends on the initial guess.

The reading is not that mixtures should not be used. It is that the class’s cost is one order lower than the audit shows: the distortion figures are the visible price, and the loss of a formula is the invisible one, paid by every consumer downstream of the map rather than by the person who designed it.

Where this ladder goes

Two constraints on that larger search are already established. Chebyshev’s criterion gives the exact answer for the conformal maps of a region, so the conformal subspace is solved and mixing within it gains nothing. And a mixture across aspects can fold, so the search space is not simply connected in any useful sense.

What is left is the space between: mixtures of non-conformal projections, over a stated region, under a stated criterion, with the fold as a constraint rather than a surprise. The next rung on this ladder is how many such maps a job needs at all, which turns out to be settled by the tolerance long before it is settled by the projection.

Named alongside this one

Essays reaching for the same objects. Nobody chose these; they are what the concept index makes visible.

What links here

Every essay whose body links to this one.

The objects this essay names

Each one links to every other essay that touches it.

Airy's criterionBlendingCompromiseConformalityEqual-areaGeneral-purpose mapJacobianObjective functionOptimisationOrientationVerificationWinkel tripel