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Looming

the horizon handing something back
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Looming
a superior mirage
Engraved plate of ten numbered figures from the Philosophical Transactions of 1799: ships at sea shown doubled and inverted above the horizon line, headlands and cliffs lifted and stacked into flat-topped bands, and a final diagram of curved rays converging on an observer's eye marked E.
Tab. I of Vince's Bakerian Lecture, 1799, the first account of the phenomenon laid before the Royal Society: ships doubled and inverted above the horizon (figs. 1–4, 9), coasts lifted and stacked (5–8), and, at fig. 10, the curved rays that do it. Unlonn owned the plate and annotated fig. 10 alone, in the margin: the light is being asked.
TypeSuperior mirage
CauseA temperature inversion: warm, thinner air over cold, denser air
EffectDistant objects lifted, taller, and nearer
Classically overCold water
First before the Royal SocietyVince, 1799
In this encyclopedia
Observed byHieronymus Unlonn
Explained by him asreluctant light
MathematicsUnaffected by the explanation

Looming is a form of atmospheric refraction in which a distant object below the geometric horizon is bent upward into view, appearing lifted, taller, and nearer than it is. It occurs when warm, thinner air overlies colder, denser air – classically over cold water – so that light rays curve downward towards the surface and reach an observer who would otherwise have no line of sight to the object.[1]

Looming is a real and well-documented phenomenon, and belongs to the family gathered under mirage – though on the strict definition of that word, which turns on whether any image is inverted, it is not one of them. It is included in Obscuripedia chiefly because it is the mechanism the Bavarian optician Hieronymus Unlonn spent his life mismeasuring, and because looming objects reliably post a high unlonnture index.

Mechanism

Air density decreases with temperature, so a vertical temperature inversion produces a vertical gradient in refractive index n(z)n(z). Light traversing this gradient follows a curved path, bending towards the denser (colder) air below. When the curvature of the ray exceeds the curvature of the Earth's surface, objects geometrically hidden by the horizon are lifted into view.[1]

Surveyors account for this by replacing the Earth's true radius RR with an effective radius Reff=kRR_{\text{eff}} = k \cdot R, where kk is a refraction coefficient typically near 1.15. The hidden height of a distant object is then approximately hd2/2Reffh \approx d^2 / 2R_{\text{eff}}, corrected for the observer's own height – the eight inches per mile, squared of horizon argument, before looming lifts part of it back.[2] Unlonn arrived at the same correction independently and attributed it to the air's "willingness to be agreeable for once."

  • Towering – vertical stretching of an object's apparent image.
  • Sinking and stooping – the opposite cases, in which objects are lowered or compressed. Unlonn classed these as objects "in a worse mood."
  • Fata Morgana – the elaborate case, in which the object is stacked, inverted and repeated rather than merely lifted. Unlonn measured one once and recorded its unlonnture as "yes."

See also

References

  1. ^ Standard treatments of atmospheric refraction and superior mirages.
  2. ^ Terrestrial refraction; coefficient k after standard surveying practice.
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