A chart represents a curved surface on a flat page. Before interpreting a straight route line, ask two questions: what does the projection do to the meridians, and which sort of route does a straight line represent?
Local north changes along a route
Each position has its own meridian and its own direction of true north. On a sphere, travelling along a great circle generally changes the angle between the route and that local north. Meridians are not globally parallel; they meet at the poles.
For a modest longitude interval within one latitude band, the familiar navigation approximation is:
convergency ≈ longitude difference × sin(mean latitude)
Use degrees consistently. This is a local approximation for route calculations, not an exact great-circle bearing formula for every pair of coordinates. The corresponding differential relationship explains why the effect is small near the equator and larger toward a pole.
Rhumb lines and great circles
A rhumb line keeps one true track angle as it crosses successive meridians. East–west travel along a parallel is an example. In still air, holding the corresponding true heading follows that route; wind requires a heading correction.
A great-circle arc follows a plane through the centre of a spherical Earth. The shorter arc gives the minimum spherical distance between non-antipodal endpoints. Except for special cases such as equatorial or meridional travel, its track angle changes en route.
The conversion angle at an endpoint compares the great-circle track there with the rhumb-line track connecting the same endpoints. For a short same-latitude leg, half the approximate convergency is a useful estimate. With large separations or unequal latitudes, calculate the endpoint bearings instead of assuming that both endpoint corrections are identical.
What changes on a Mercator chart
On the normal Mercator projection, meridians appear as parallel vertical lines. A rhumb line is straight, and most great-circle routes are curved. The equator and meridians are exceptions: they can represent both kinds of route.
The map stretches high latitudes. For an equator-scaled spherical Mercator, local scale grows as 1 / cos(latitude). At 60°, the scale factor is two. The geographic poles cannot be drawn at a finite distance on this projection. A visually short line on the map therefore need not represent the shortest surface route.
What changes on a Lambert conformal conic chart
Lambert meridians radiate from a common point. Chart convergence equals longitude difference × n, where n is the cone constant. For a tangent spherical construction at latitude φ, n = sin φ. A secant construction with two standard parallels has its own cone constant; do not simply substitute their arithmetic mean as an exact rule.
Across a suitably chosen regional Lambert chart, a straight route line is a useful approximation to a great circle. Neither all distances nor every great-circle route becomes exact. Read the chart's projection and standard parallels rather than assuming a projection from its aviation use.
- Meridians: parallel vertical lines
- Chart convergency: 0
- Best for equatorial belt
- Meridians: radiate from apex
- Chart convergence ≈ Earth convergency
- Best for mid-latitude topographical charts
- Meridians: radiate from pole
- Great circles ≈ straight (exact at pole)
- Best above 70° latitude
A small-leg calculation
Consider two study points at 50°N, one at 002°W and the other at 008°E. Their longitude separation is 10° and the eastbound rhumb-line track is 090°T.
- Approximate convergency: 10 × sin 50° ≈ 7.66°.
- Approximate endpoint conversion angle: 7.66 / 2 ≈ 3.83°.
- The eastbound great circle initially runs slightly toward the nearer pole: 090 − 3.83 ≈ 086.17°T.
- By arrival it runs slightly away from that pole: 090 + 3.83 ≈ 093.83°T.
The exact spherical initial bearing is about 086.166°T, so the approximation works well for this example. That agreement does not justify extending the shortcut across an ocean or across the equator without checking the geometry. The widgets illustrate the relationships; use exact spherical calculations or approved planning tools when the approximation is unsuitable.
Common checks
- Specify which endpoint a bearing describes. The reciprocal of an initial outbound bearing is not generally the initial bearing for the entire return great-circle route.
- Distinguish chart convergence from the route's changing true track. They belong to different geometries.
- Treat a projection diagram as a way of understanding the mathematics, not as a literal light projection that constructs every conformal map.
Further reading
USGS: map projections and their properties and FAA Aeronautical Chart Users' Guide. The short-leg example is calculated for this lesson on a spherical Earth.