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How far away is the horizon?

About 4.7 kilometres. That is how far away the horizon is when you stand on a beach and look out to sea. It feels like the edge of the world should be further — but the Earth curves away from you surprisingly quickly, and with one right-angled triangle and Pythagoras' theorem we can work out exactly where your view runs out. Let's derive it for ourselves.

The geometry: one tangent line

Your line of sight to the horizon is the line that just grazes the Earth's surface — in the language of circle theorems, a tangent. And a tangent to a circle meets the radius at the point of contact at exactly 9090^\circ. That single fact hands us a right-angled triangle:

Right-angled triangle formed by the Earth's radius, the sightline to the horizon, and the line from the Earth's centre to the observer's eye

The three sides are: the Earth's radius RR out to the horizon point, your sightline of length dd, and the hypotenuse from the Earth's centre up to your eye, of length R+hR + h, where hh is the height of your eye above the surface. Pythagoras' theorem then says:

(R+h)2=R2+d2(R+h)^2 = R^2 + d^2

Solving for dd and expanding the bracket:

d=(R+h)2R2=2Rh+h2d = \sqrt{(R+h)^2 - R^2} = \sqrt{2Rh + h^2}

Now for a lovely simplification. Because hh is tiny compared with RR, the h2h^2 term is negligible: for a person with eye height h=1.7h = 1.7 m, 2Rh2Rh is about 21.7 million m², while h2h^2 is just 2.9 m². Dropping it:

d2Rhd \approx \sqrt{2Rh}

One radius, one height, one square root.

We take R=6,371,000R = 6{,}371{,}000 m [1] and work in metres throughout.

  1. Standing on the beach, eye height h=1.7h = 1.7 m:
d2×6,371,000×1.74,650 m4.7 kmd \approx \sqrt{2 \times 6{,}371{,}000 \times 1.7} \approx 4{,}650 \text{ m} \approx 4.7 \text{ km}
  1. On a 100 m cliff top:
d2×6,371,000×10035,700 m36 kmd \approx \sqrt{2 \times 6{,}371{,}000 \times 100} \approx 35{,}700 \text{ m} \approx 36 \text{ km}
  1. From a plane cruising at 11,000 m:
d2×6,371,000×11,000374,000 m374 kmd \approx \sqrt{2 \times 6{,}371{,}000 \times 11{,}000} \approx 374{,}000 \text{ m} \approx 374 \text{ km}

(Even at aeroplane height our approximation holds up: the exact formula gives 374.5 km, a difference of only 0.04%.) Notice the square root at work: multiplying your height by 4 only doubles your view. That is exactly why sailors climbed to the crow's nest — every metre of mast bought a disproportionately useful amount of extra horizon.

The same geometry explains a phenomenon observed for millennia. A ship sailing away doesn't shrink to a dot and fade — it sinks below the horizon, hull first, while the masts stay visible longest. Once the ship passes your tangent point, the bulge of the Earth stands between your eye and the ship's waterline, but the taller parts still poke above your grazing sightline:

A ship beyond the horizon with its hull hidden by the Earth's curvature while the masts remain visible above the tangent sightline

Long before satellites, this was everyday evidence that the sea is curved — the very curvature that a stick in Alexandria measured 2,200 years ago.

What the atmosphere adds

With one circle theorem and Pythagoras, we found d2Rhd \approx \sqrt{2Rh}: about 4.7 km from the beach, 36 km from a 100 m cliff, and 374 km from a cruising aeroplane. Our model is honest but simplified. Real air bends light: the atmosphere's density gradient refracts your sightline slightly around the curve, extending the visible horizon by roughly 8% under standard conditions — navigators' handbooks bake this correction into their tables [2]. We have also ignored waves, tides and the Earth's slight squashedness. Still, next time you're at the beach, you can point at the horizon and say precisely how far you're looking — and know the square root that put it there.


References:

[1] NASA Goddard Space Flight Center: Earth Fact Sheet

[2] Nathaniel Bowditch, The American Practical Navigator (National Geospatial-Intelligence Agency, Bethesda).

Note: All distances assume a smooth, spherical Earth and neglect atmospheric refraction, which in practice pushes the horizon a little further than the pure geometry suggests.