Labels | Values | formula | ||||||
R, radius of Earth (miles) | 3963 | |||||||
D, distance from observer (miles) | 60 | |||||||
α, angle to observer (radians) | 0.015140045 | D / R | ||||||
A | 3962.545807 | R ∙ cos(α) | ||||||
B | 59.99770782 | R ∙ sin(α) | ||||||
C | 0.454192687 | R - A | ||||||
E | 59.99942695 | sqrt(B²+C²) | ||||||
F | 29.99971347 | E / 2 | ||||||
G | 3962.88645 | sqrt(R²-F²) | ||||||
H | 0.113549798 | R - G | ||||||
H in feet | 599.5429355 | H x 5280 ft/mi | ||||||
Calculate the height of the effective barrier between observer and object under observation, created by the | ||||||||
curvature of the Earth, as a function of the distance between observer and object under observation. | ||||||||
I.e., calculate the maximum height difference between a straight line and a curve which follows the curvature | ||||||||
of the Earth. | ||||||||
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The fundamental deficiency in this approach is the assumption that Earth has no atmosphere. | ||||||||
In the real world, the Earth's atmosphere acts as a lens, which refracts light. Depending | ||||||||
on atmospheric conditions, it is often possible for things beneath the horizon to appear at | ||||||||
the horizon, or even above the horizon. Here are a couple of very good web pages on this topic: | ||||||||
http://www-rohan.sdsu.edu/~aty/explain/atmos_refr/horizon.html | ||||||||
http://www-rohan.sdsu.edu/~aty/explain/atmos_refr/altitudes.html |
Dave Burton
30 April, 2016