How the Flat vs. Round Earth Calculator Works
On a sphere, a level line of sight from your eye is tangent to the surface — it touches the globe at exactly one point (your horizon) and then rises above the ground beyond it. That means a distant object doesn't just shrink evenly with distance the way it would over a flat plane; once it passes beyond your horizon, its base disappears first while its upper portion stays visible a little longer. This calculator uses the same spherical-geometry formulas that surveyors, sailors, and lighthouse engineers use to compute your horizon distance, how far the surface has "dropped" below a level line at any distance, and how much of a distant object of known height would be hidden below that horizon.
Deriving the formulas
Picture a right triangle formed by Earth's center, your eye at height h above the surface, and the point where your line of sight just grazes the horizon. The hypotenuse is R + h (Earth's radius plus your eye height), one leg is R (the radius to the horizon point), and the remaining leg is the horizon distance d — so by the Pythagorean theorem, d = √((R + h)² − R²). The curvature drop — how far the surface has fallen below a level tangent line over a distance d — comes from the same triangle in reverse: drop = R(1 − cos(d/R)), which reduces to the familiar approximation drop ≈ d² / (2R) for distances that are small compared to Earth's radius. To find how much of a distant object is hidden, the calculator applies that same drop formula starting from your horizon point rather than from your eye, since your line of sight is itself tangent to the globe at that point.
Refraction, limits, and what this doesn't model
Earth's atmosphere bends light slightly downward as it travels near the surface, letting you see a bit farther than pure geometry predicts. The standard approximation multiplies the effective Earth radius by about 7/6 (equivalent to a refraction coefficient k ≈ 0.13) to account for this under typical conditions — toggle it off to see the plain geometric numbers instead. This model assumes a clear line of sight over water or flat terrain with no obstructions, and it doesn't account for temperature-inversion mirages, which can occasionally make refraction unusually strong or weak and let objects appear higher or lower than the standard formula predicts. It's also a small-angle approximation meant for line-of-sight distances up to a few hundred kilometers, not for antipodal-scale distances where the flat tangent-line picture breaks down entirely.