This projection

is another conventional projection, neither conformal nor equal-area.

Like the globular projection, this projection is constructed by drawing circular arcs for both the meridians and the parallels. However, while the globular projection serves as a simpler-to-draw replacement for the equatorial case of the azimuthal equidistant, a compromise about midway between conformality and equivalence, this projection has an obvious strong resemblance to the Mercator. Thus, while it is intended to moderate, slightly, the exaggeration of areas of the Mercator, and to provide a pleasing appearance with curved meridians and parallels, it definitely favors shapes at the expense of areas. (Again, it is not strictly conformal, but the Lagrange projection, which is somewhat similar in appearance, is.)

In fact, to realize that it even moderates areas at all compared to the Mercator, one must make a direct comparison:

If anything, given that its curved parallels and meridians may give it the appearance of truth, this projection might be viewed as even more dangerously misleading than the Mercator.

The meridians are constructed exactly as in the globular projection, except that the equator is now divided into 360 degrees instead of 180.

For the parallels, a simple geometrical construction determines where each parallel cuts the surrounding circle and the central meridian.

Divide the height of the projection uniformly to indicate latitude, as shown by the blue lines. Then, where a line (shown as red in the diagram) drawn from the bounding circle at the height corresponding to a given latitude to the point where the other side of the bounding circle intersects the equator intersects the central meridian is where the parallel for that latitude crosses the central meridian.

The height at which the parallel for that latitude intersects the bounding circle is found in a similar fashion. Here, however, instead of the bounding circle, one uses a diagonal line (shown in green) between a pole of the projection and a point where the bounding circle crosses the equator. A line (shown as purple) is drawn from the point on this diagonal line at the height determined by the uniform division of the height of the projection and corresponding to the desired latitude, again to the point where the bounding circle crosses the equator at the other side. The height of the point where this line crosses the central meridian is the height at which the parallel, as drawn on the actual map, intersects the bounding circle.

For serious cartographic applications, it is natural to entertain serious doubt about the utility of this projection. It doesn't have the useful property of strict conformality, and, without that excuse, it would seem impossible to justify the exaggeration of areas in this projection. Other near-Mercator projections, like the Miller Cylindrical, are perhaps forced to exaggerate areas because they are cylindrical, therefore preserving the four cardinal compass points in conventional aspect.

However, the achievement of van der Grinten in so closely approaching conformality in a projection with such a simple construction is still one that is worthy of praise. At the least, given the familiarity of the Mercator projection, this projection seems to be an excellent choice as a map of the world for decorative purposes.

The van der Grinten III projection, where the parallels are simply straight lines with the spacing given in the center of the projection, has also been popular, even though the graticule of the entire projection looks somewhat strange. This projection is also known as the Brooks-Roberts projection. It works quite well, as long as the polar regions of the map are excluded.

Every now and then, I have seen maps that look very much like the normal van der Grinten projection, but which are labelled as being drawn on a "Modified van der Grinten Projection". Given that the van der Grinten III projection seems to work well, perhaps a suitable modification of the van der Grinten might be to change the point at which the parallels intersect the boundary of the projection to a weighted average of three parts the original boundary height, and one part the center height, giving the following projection:

It might seem there is no difference, but if you look closely at how Alaska appears in the modified projection and the original, it seems that a tiny improvement has been achieved.

And a direct overlay also allows the very subtle difference to be seen:

Although this is a conventional projection, and therefore an oblique aspect is not really applicable to such projections, because an oblique aspect gives a different perspective on a projection, it allows its distortions to be perhaps more readily seen. Thus, here is this modified form of the Van der Grinten projection in the oblique aspect used in other examples on these pages:

Given that it so closely approaches conformality, it seemed worthwhile to ask if applying a conformal transformation to the world so that a hemisphere could be placed within a van der Grinten projection (superimposing a double-sized Mercator over one at normal scale) would produce an attractive projection. This is the result:

A projection is obtained which resembles the globular projection, but which has a slight expansion of scale along the central meridian towards the poles.