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Atmospheric optics
Atmospheric optics
from Wikipedia
A colorful sky is often due to indirect sunlight being scattered off air molecules and particulates, like smog, soot, and cloud droplets, as shown in this photo of a sunset during the October 2007 California wildfires.

Atmospheric optics is "the study of the optical characteristics of the atmosphere or products of atmospheric processes .... [including] temporal and spatial resolutions beyond those discernible with the naked eye".[1] Meteorological optics is "that part of atmospheric optics concerned with the study of patterns observable with the naked eye".[2] Nevertheless, the two terms are sometimes used interchangeably.

Meteorological optical phenomena, as described in this article, are concerned with how the optical properties of Earth's atmosphere cause a wide range of optical phenomena and visual perception phenomena. Examples of meteorological phenomena include:

  • The blue color of the sky. This is from Rayleigh scattering, which sends more higher frequency/shorter wavelength (blue) sunlight into the eye of an observer than other frequencies/wavelength.
  • The reddish color of the Sun when it is observed through a thick atmosphere, as during a sunrise or sunset. This is because long-wavelength (red) light is scattered less than blue light. The red light reaches the observer's eye, whereas the blue light is scattered out of the line of sight.
  • Other colours in the sky, such as glowing skies at dusk and dawn. These are from additional particulate matter in the sky that scatter different colors at different angles.
  • Halos, afterglows, coronas, polar stratospheric clouds, and sun dogs. These are from scattering, or refraction, by ice crystals and from other particles in the atmosphere. They depend on different particle sizes and geometries.[3]
  • Mirages. These are optical phenomena in which light rays are bent due to thermal variations in the refractive index of air, producing displaced or heavily distorted images of distant objects. Other optical phenomena associated with this include the Novaya Zemlya effect, in which the Sun has a distorted shape and rises earlier or sets later than predicted. A spectacular form of refraction, called the Fata Morgana, occurs with a temperature inversion, in which objects on the horizon or even beyond the horizon (e.g. islands, cliffs, ships, and icebergs) appear elongated and elevated, like "fairy tale castles".[4]
  • Rainbows. These result from a combination of internal reflection and dispersive refraction of light in raindrops. Because rainbows are seen on the opposite side of the sky from the Sun, rainbows are more visible the closer the Sun is to the horizon. For example, if the Sun is overhead, any possible rainbow appears near an observer's feet, making it hard to see, and involves very few raindrops between the observer's eyes and the ground, making any rainbow very sparse.[5]

Other phenomena that are remarkable because they are forms of visual illusions include:

History

[edit]

A book on meteorological optics was published in the sixteenth century, but there have been numerous books on the subject since about 1950.[6] The topic was popularised by the wide circulation of a book by Marcel Minnaert, Light and Color in the Open Air, in 1954.[7][8]

Sun and Moon size

[edit]
Comparison between the relative sizes of the Moon and a cloud at different points in the sky

In the Book of Optics (1011–22 AD), Ibn al-Haytham argued that vision occurs in the brain, and that personal experience has an effect on what people see and how they see, and that vision and perception are subjective. Arguing against Ptolemy's refraction theory for why people perceive the Sun and Moon larger at the horizon than when they are higher in the sky, he redefined the problem in terms of perceived, rather than real, enlargement. He said that judging the distance of an object depends on there being an uninterrupted sequence of intervening bodies between the object and the observer. Critically, Ibn al-Haytham said that judging the size of an object depends on its judged distance: an object that appears near appears smaller than an object having the same image size on the retina that appears far. With the overhead Moon, there is no uninterrupted sequence of intervening bodies. Hence it appears far and small. With a horizon Moon, there is an uninterrupted sequence of intervening bodies: all the objects between the observer and the horizon, so the Moon appears far and large. Through works by Roger Bacon, John Pecham, and Witelo based on Ibn al-Haytham's explanation, the Moon illusion gradually came to be accepted as a psychological phenomenon, with Ptolemy's theory being rejected in the 17th century.[9] For over 100 years, research on the Moon illusion has been conducted by vision scientists who invariably have been psychologists specializing in human perception. After reviewing the many different explanations in their 2002 book The Mystery of the Moon Illusion, Ross and Plug concluded "No single theory has emerged victorious".[10]

Sky coloration

[edit]
When seen from a high altitude, as here from an airplane, the sky's color varies from pale to dark at elevations toward the zenith.

The color of light from the sky is a result of Rayleigh scattering of sunlight, which results in a perceived blue color. On a sunny day, Rayleigh scattering gives the sky a blue gradient, darkest around the zenith and brightest near the horizon. Light rays coming from the zenith take the shortest-possible path (138) through the air mass, yielding less scattering. Light rays coming from the horizon take the longest-possible path through the air, yielding more scattering.[11]

The blueness is at the horizon because the blue light coming from great distances is also preferentially scattered. This results in a red shift of the distant light sources that is compensated by the blue hue of the scattered light in the line of sight. In other words, the red light scatters also; if it does so at a point a great distance from the observer it has a much higher chance of reaching the observer than blue light. At distances nearing infinity, the scattered light is therefore white. Distant clouds or snowy mountaintops will seem yellow for that reason;[12] that effect is not obvious on clear days, but very pronounced when clouds are covering the line of sight reducing the blue hue from scattered sunlight.

The scattering due to molecule sized particles (as in air) is greater in the forward and backward directions than it is in the lateral direction.[13] Individual water droplets exposed to white light will create a set of colored rings. If a cloud is thick enough, scattering from multiple water droplets will wash out the set of colored rings and create a washed out white color.[14] Dust from the Sahara moves around the southern periphery of the subtropical ridge moves into the southeastern United States during the summer, which changes the sky from a blue to a white appearance and leads to an increase in red sunsets. Its presence negatively affects air quality during the summer since it adds to the count of airborne particulates.[15]

Purple sky on the La Silla Observatory.[16]

The sky can turn a multitude of colors such as red, orange, pink and yellow (especially near sunset or sunrise) and black at night. Scattering effects also partially polarize light from the sky, most pronounced at an angle 90° from the Sun.

Sky luminance distribution models have been recommended by the International Commission on Illumination (CIE) for the design of daylighting schemes. Recent developments relate to “all sky models” for modelling sky luminance under weather conditions ranging from clear sky to overcast.[17]

Cloud coloration

[edit]
An occurrence of altocumulus and cirrocumulus cloud iridescence
Sunset reflecting shades of pink onto grey stratocumulus clouds.

The color of a cloud, as seen from the Earth, tells much about what is going on inside the cloud. Dense deep tropospheric clouds exhibit a high reflectance (70% to 95%) throughout the visible spectrum. Tiny particles of water are densely packed and sunlight cannot penetrate far into the cloud before it is reflected out, giving a cloud its characteristic white color, especially when viewed from the top.[18] Cloud droplets tend to scatter light efficiently, so that the intensity of the solar radiation decreases with depth into the gases. As a result, the cloud base can vary from a very light to very dark grey depending on the cloud's thickness and how much light is being reflected or transmitted back to the observer. Thin clouds may look white or appear to have acquired the color of their environment or background. High tropospheric and non-tropospheric clouds appear mostly white if composed entirely of ice crystals and/or supercooled water droplets.

As a tropospheric cloud matures, the dense water droplets may combine to produce larger droplets, which may combine to form droplets large enough to fall as rain. By this process of accumulation, the space between droplets becomes increasingly larger, permitting light to penetrate farther into the cloud. If the cloud is sufficiently large and the droplets within are spaced far enough apart, it may be that a percentage of the light which enters the cloud is not reflected back out before it is absorbed. A simple example of this is being able to see farther in heavy rain than in heavy fog. This process of reflection/absorption is what causes the range of cloud color from white to black.[19]

Other colors occur naturally in clouds. Bluish-grey is the result of light scattering within the cloud. In the visible spectrum, blue and green are at the short end of light's visible wavelengths, while red and yellow are at the long end.[20] The short rays are more easily scattered by water droplets, and the long rays are more likely to be absorbed. The bluish color is evidence that such scattering is being produced by rain-sized droplets in the cloud. A cumulonimbus cloud emitting green is a sign that it is a severe thunderstorm,[21] capable of heavy rain, hail, strong winds and possible tornadoes. The exact cause of green thunderstorms is still unknown, but it could be due to the combination of reddened sunlight passing through very optically thick clouds. Yellowish clouds may occur in the late spring through early fall months during forest fire season. The yellow color is due to the presence of pollutants in the smoke. Yellowish clouds caused by the presence of nitrogen dioxide are sometimes seen in urban areas with high air pollution levels.[22]

Red, orange and pink clouds occur almost entirely at sunrise and sunset and are the result of the scattering of sunlight by the atmosphere. When the angle between the Sun and the horizon is less than 10 percent, as it is just after sunrise or just prior to sunset, sunlight becomes too red due to refraction for any colors other than those with a reddish hue to be seen.[21] The clouds do not become that color; they are reflecting long and unscattered rays of sunlight, which are predominant at those hours. The effect is much like if a person were to shine a red spotlight on a white sheet. In combination with large, mature thunderheads this can produce blood-red clouds. Clouds look darker in the near-infrared because water absorbs solar radiation at those wavelengths.

Halo

[edit]
A 22° halo around the Sun, observed over Bretton Woods, New Hampshire, USA on February 13, 2021

A halo (ἅλως; also known as a nimbus, icebow or gloriole) is an optical phenomenon produced by the interaction of light from the Sun or Moon with ice crystals in the atmosphere, resulting in colored or white arcs, rings or spots in the sky.[23] Many halos are positioned near the Sun or Moon, but others are elsewhere and even in the opposite part of the sky. They can also form around artificial lights in very cold weather when ice crystals called diamond dust are floating in the nearby air.[24]

There are many types of ice halos. They are produced by the ice crystals in cirrus or cirrostratus clouds high in the upper troposphere, at an altitude of 5 kilometres (3.1 mi) to 10 kilometres (6.2 mi), or, during very cold weather, by ice crystals called diamond dust drifting in the air at low levels.[25][26][27] The particular shape and orientation of the crystals are responsible for the types of halo observed. Light is reflected and refracted by the ice crystals and may split into colors because of dispersion. The crystals behave like prisms and mirrors, refracting and reflecting sunlight between their faces, sending shafts of light in particular directions.[23] For circular halos, the preferred angular distance are 22 and 46 degrees from the ice crystals which create them.[28] Atmospheric phenomena such as halos have been used as part of weather lore as an empirical means of weather forecasting, with their presence indicating an approach of a warm front and its associated rain.[29]

Sun dogs

[edit]
Very bright sundogs in Fargo, North Dakota. Note the halo arcs passing through each sun dog.

Sun dogs are a common type of halo, with the appearance of two subtly-colored bright spots to the left and right of the Sun, at a distance of about 22° and at the same elevation above the horizon. They are commonly caused by plate-shaped hexagonal ice crystals.[25][26] These crystals tend to become horizontally aligned as they sink through the air, causing them to refract the sunlight to the left and right, resulting in the two sun dogs.[26][25]

As the Sun rises higher, the rays passing through the crystals are increasingly skewed from the horizontal plane. Their angle of deviation increases and the sundogs move further from the Sun.[30] However, they always stay at the same elevation as the Sun. Sun dogs are red-colored at the side nearest the Sun. Farther out the colors grade to blue or violet.[25] However, the colors overlap considerably and so are muted, rarely pure or saturated. The colors of the sun dog finally merge into the white of the parhelic circle (if the latter is visible).

It is theoretically possible to predict the forms of sun dogs as would be seen on other planets and moons. Mars might have sundogs formed by both water-ice and CO2-ice. On the giant gas planets — Jupiter, Saturn, Uranus and Neptune — other crystals form the clouds of ammonia, methane, and other substances that can produce halos with four or more sundogs.[31]

Glory

[edit]
Solar glory at the steam from a hot spring

A common optical phenomenon involving water droplets is the glory.[23] A glory is an optical phenomenon, appearing much like an iconic Saint's halo about the head of the observer, produced by light backscattered (a combination of diffraction, reflection and refraction) towards its source by a cloud of uniformly sized water droplets. A glory has multiple colored rings, with red colors on the outermost ring and blue/violet colors on the innermost ring.[32]

The angular distance is much smaller than a rainbow, ranging between 5° and 20°, depending on the size of the droplets. The glory can only be seen when the observer is directly between the Sun and cloud of refracting water droplets. Hence, it is commonly observed while airborne, with the glory surrounding the airplane's shadow on clouds (this is often called The Glory of the Pilot). Glories can also be seen from mountains and tall buildings,[33] when there are clouds or fog below the level of the observer, or on days with ground fog. The glory is related to the optical phenomenon anthelion.

Rainbow

[edit]
Double rainbow and supernumerary rainbows on the inside of the primary arc. The shadow of the photographer's head marks the centre of the rainbow circle (antisolar point).

A rainbow is a narrow, multicoloured semicircular arc due to dispersion of white light by a multitude of drops of water, usually in the form of rain, when they are illuminated by sunlight. Hence, when conditions are right, a rainbow always appears in the section of sky directly opposite the Sun. For an observer on the ground, the amount of the arc that is visible depends on the height of the sun above the horizon. It is a full semicircle with an angular radius of 42° when the sun is at the horizon. But as the sun rises in the sky, the arc grows smaller and ceases to be visible when the sun is more than 42° above the horizon. To see more than a semicircular bow, an observer would have to be able to look down on the drops, say from an airplane or a mountaintop. Rainbows are most common during afternoon rain showers in summer.[34]

A single reflection off the backs of an array of raindrops produces a rainbow with an angular size that ranges from 40° to 42° with red on the outside and blue/violet on the inside. This is known as the primary bow. A fainter secondary bow is often visible some 10° outside the primary bow. It is due to two internal reflections within a drop. The resulting secondary arc is some 3° wide and the colours are reversed, with blue/violet on the outside. Two internal reflections produce a bow with angular size of 50.5° to 54° with blue/violet on the outside.[34] The region between a double rainbow is often noticeably darker that the sky within the primary bow and that beyond the secondary bow. It known an Alexander's Dark Band. The reason for this apparent reduction in sky brightness is that, while light from the sky enclosed within the primary bow comes from droplet reflection, and light beyond the secondary bow also comes from droplet reflection, there is no mechanism for the region between the bows to reflect light in the direction of the observer. Generally speaking, larger the droplets make for brighter bows.

A rainbow spans a continuous spectrum of colors; the distinct bands (including the number of bands) are an artifact of human color vision, and no banding of any type is seen in a black-and-white photograph of a rainbow (only a smooth gradation of intensity to a maxima, then fading to a minima at the other side of the arc). For colors seen by a normal human eye, the most commonly cited and remembered sequence, in English, is Isaac Newton's sevenfold red, orange, yellow, green, blue, indigo and violet (popularly memorized by mnemonics like Roy G. Biv).[35]

Mirage

[edit]
Various kinds of mirages in one location taken over the course of six minutes. The uppermost inset frame shows an inferior mirage of the Farallon Islands. The second inset frame shows a green flash on the left-hand side. The two lower frames and the main frame all show superior mirages of the Farallon Islands. In these three frames, the superior mirage evolves from a 3-image mirage to a 5-image mirage, and back to a 2-image mirage. Such a display is consistent with a Fata Morgana.

A mirage is a naturally occurring optical phenomenon in which light rays are bent to produce a displaced image of distant objects or the sky. The word comes to English via the French mirage, from the Latin mirare, meaning "to look at, to wonder at". This is the same root as for "mirror" and "to admire". Also, it has its roots in the Arabic mirage.

In contrast to a hallucination, a mirage is a real optical phenomenon which can be captured on camera, since light rays actually are refracted to form the false image at the observer's location. What the image appears to represent, however, is determined by the interpretive faculties of the human mind. For example, inferior images on land are very easily mistaken for the reflections from a small body of water.

Mirages can be categorized as "inferior" (meaning lower), "superior" (meaning higher) and "Fata Morgana", one kind of superior mirage consisting of a series of unusually elaborate, vertically stacked images, which form one rapidly changing mirage.

Green flashes and green rays are optical phenomena that occur shortly after sunset or before sunrise, when a green spot is visible, usually for no more than a second or two, above the Sun, or a green ray shoots up from the sunset point. Green flashes are actually a group of phenomena stemming from different causes, and some are more common than others.[36] Green flashes can be observed from any altitude (even from an aircraft). They are usually seen at an unobstructed horizon, such as over the ocean, but are possible over cloud tops and mountain tops as well.

A green flash from the Moon and bright planets at the horizon, including Venus and Jupiter, can also be observed.[37][38]

Fata Morgana

[edit]
A Fata Morgana of a boat

This optical phenomenon occurs because rays of light are strongly bent when they pass through air layers of different temperatures in a steep thermal inversion where an atmospheric duct has formed.[39] A thermal inversion is an atmospheric condition where warmer air exists in a well-defined layer above a layer of significantly cooler air. This temperature inversion is the opposite of what is normally the case; air is usually warmer close to the surface, and cooler higher up. In calm weather, a layer of significantly warmer air can rest over colder dense air, forming an atmospheric duct which acts like a refracting lens, producing a series of both inverted and erect images.

A Fata Morgana is an unusual and very complex form of mirage, a form of superior mirage, which, like many other kinds of superior mirages, is seen in a narrow band right above the horizon. It is an Italian phrase derived from the vulgar Latin for "fairy" and the Arthurian sorcerer Morgan le Fay,[40] from a belief that the mirage, often seen in the Strait of Messina, were fairy castles in the air,[41] or false land designed to lure sailors to their death created by her witchcraft. Although the term Fata Morgana is sometimes incorrectly applied to other, more common kinds of mirages, the true Fata Morgana is not the same as an ordinary superior mirage, and is certainly not the same as an inferior mirage.

Fata Morgana mirages tremendously distort the object or objects which they are based on, such that the object often appears to be very unusual, and may even be transformed in such a way that it is completely unrecognizable. A Fata Morgana can be seen on land or at sea, in polar regions or in deserts. This kind of mirage can involve almost any kind of distant object, including such things as boats, islands, and coastline.

A Fata Morgana is not only complex, but also rapidly changing. The mirage comprises several inverted (upside down) and erect (right side up) images that are stacked on top of one another. Fata Morgana mirages also show alternating compressed and stretched zones.[39]

Novaya Zemlya effect

[edit]

The Novaya Zemlya effect is a polar mirage caused by high refraction of sunlight between atmospheric thermoclines. The Novaya Zemlya effect will give the impression that the sun is rising earlier or setting later than it actually should (astronomically speaking).[42] Depending on the meteorological situation the effect will present the Sun as a line or a square (which is sometimes referred to as the "rectangular sun"), made up of flattened hourglass shapes. The mirage requires rays of sunlight to have an inversion layer for hundreds of kilometres, and depends on the inversion layer's temperature gradient. The sunlight must bend to the Earth's curvature at least 400 kilometres (250 mi) to allow an elevation rise of 5 degrees for sight of the sun disk.

The first person to record the phenomenon was Gerrit de Veer, a member of Willem Barentsz' ill-fated third expedition into the polar region. Novaya Zemlya, the archipelago where de Veer first observed the phenomenon, lends its name to the effect.[42]

Crepuscular rays

[edit]
Crepuscular rays, taken in Taipei, Taiwan.

Crepuscular rays are near-parallel rays of sunlight moving through the Earth's atmosphere, but appear to diverge because of linear perspective.[43] They often occur when objects such as mountain peaks or clouds partially shadow the Sun's rays like a cloud cover. Various airborne compounds scatter the sunlight and make these rays visible, due to diffraction, reflection, and scattering.

Crepuscular rays can also occasionally be viewed underwater, particularly in arctic areas, appearing from ice shelves or cracks in the ice. Also they are also viewed in days when the sun hits the clouds in a perfect angle shining upon the area.

There are three primary forms of crepuscular rays[citation needed]:

  • Rays of light penetrating holes in low clouds (also called "Jacob's Ladder").
  • Beams of light diverging from behind a cloud.
  • Pale, pinkish or reddish rays that radiate from below the horizon. These are often mistaken for light pillars.

They are commonly seen near sunrise and sunset, when tall clouds such as cumulonimbus and mountains can be most effective at creating these rays.[citation needed]

Anticrepuscular rays

[edit]

Anticrepuscular rays while parallel in reality are sometimes visible in the sky in the direction opposite the sun. They appear to converge again at the distant horizon.

Atmospheric refraction

[edit]
Diagram showing displacement of the Sun's image at sunrise and sunset

Atmospheric refraction influences the apparent position of astronomical and terrestrial objects, usually causing them to appear higher than they actually are. For this reason navigators, astronomers, and surveyors observe positions when these effects are minimal. Sailors will only shoot a star when 20° or more above the horizon, astronomers try to schedule observations when an object is highest in the sky, and surveyors try to observe in the afternoon when refraction is minimum.

Atmospheric diffraction

[edit]

Atmospheric diffraction is a visual effect caused when sunlight is bent by particles suspended in the air.

List

[edit]
A circumzenithal arc over Grand Forks, North Dakota
The Belt of Venus over Paranal Observatory atop Cerro Paranal in the Atacama Desert, northern Chile[44]
Crepuscular rays at sunrise in Malibu, California

Atmospheric optical phenomena include:

A double rainbow at Minsi Lake, Pennsylvania
Atmospheric optical phenomenon

See also

[edit]

References

[edit]
Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Atmospheric optics is the of how interacts with Earth's atmosphere, producing a range of visual phenomena through processes such as , , reflection, , and absorption by atmospheric particles, gases, droplets, and crystals. These interactions occur when or encounters components like air molecules, aerosols, clouds, and hydrometeors, resulting in displays visible from the ground or . The fundamental processes driving atmospheric optics include , where smaller particles like air molecules preferentially scatter shorter blue wavelengths, explaining the sky's color during the day, while longer red wavelengths dominate at sunset due to increased path length through the atmosphere. Larger particles, such as cloud droplets, cause , which scatters all visible wavelengths equally, rendering clouds white or gray. and dispersion bend and separate light rays, as seen in rainbows formed by sunlight entering raindrops, undergoing internal reflection, and exiting at specific angles—primary rainbows at about 42° with red on the outer edge and violet inner, while secondary rainbows appear fainter at 50–53° with reversed colors. Notable phenomena also encompass ice crystal effects, such as halos—rings around the sun or moon, like the common caused by through hexagonal prisms in high-altitude cirrus clouds—and sundogs (parhelia), bright colored spots at 22° from the sun due to horizontal plate crystals. Mirages arise from in temperature gradients, creating illusions like inferior mirages over hot surfaces or superior mirages inverting distant objects. Other displays include (diffraction rings around the moon from thin clouds), glories (concentric rings opposite the sun from water droplets), and (beams of light through cloud gaps, appearing to converge due to perspective). Beyond aesthetics, atmospheric optics informs fields like , climate science, and , as these phenomena reveal insights into distribution, , and , influencing patterns and Earth's energy balance. Historical studies, from ' explanations of rainbows to modern models of , underscore its evolution as a bridging and .

Basic Principles

Scattering

Scattering in the atmosphere refers to the deviation of rays without absorption, primarily due to interactions with gas molecules and particles, which redirects in various directions and influences and coloration phenomena. This process is elastic, preserving the of the incident , and is fundamental to understanding how atmospheric constituents modify incoming solar radiation. Rayleigh scattering occurs when light interacts with particles much smaller than the wavelength of light, such as air molecules, resulting in elastic scattering that is highly wavelength-dependent. The scattering cross-section σ follows an inverse fourth-power dependence on wavelength λ, expressed as σ ∝ 1/λ⁴, which causes shorter wavelengths like blue to scatter more efficiently than longer ones, leading to dominance of blue light in clear skies. This relationship arises from the classical treatment of light inducing oscillating dipoles in small particles, with the scattered intensity proportional to 1/λ⁴. Mie scattering, in contrast, applies to larger particles comparable in size to the wavelength, such as aerosols or cloud droplets, and exhibits less dependence on wavelength, often producing a forward-scattering preference that results in whiter appearances for clouds and hazy conditions. Unlike Rayleigh scattering, Mie's angular distribution favors the forward direction due to diffraction effects around the particle, reducing color selectivity and scattering all visible wavelengths more uniformly. This process is described by solutions to Maxwell's equations for spherical particles, emphasizing size parameter effects where particle radius a relates to λ via x = 2πa/λ. In the Earth's atmosphere, is predominantly driven by (N₂, ~78%) and oxygen (O₂, ~21%) molecules, which are the primary scatterers due to their abundance and small size relative to visible light wavelengths. Pollution introduces additional aerosols that enhance efficiency, increasing overall and contributing to reduced in urban or industrialized areas by elevating particulate concentrations. Mathematical models of atmospheric scattering incorporate the single scattering albedo ω₀, defined as the ratio of cross-section σ_s to total cross-section (σ_s + σ_a, where σ_a is absorption), quantifying the fraction of light scattered versus absorbed; for non-absorbing Rayleigh scatterers, ω₀ ≈ 1, while aerosols may yield ω₀ < 1 due to partial absorption. The phase function p(θ) describes the angular distribution of scattered intensity, normalized such that ∫ p(θ) dΩ = 1 over the ; for , it takes the form p(θ) = (3/4)(1 + cos²θ), indicating symmetric forward-backward scattering, whereas Mie phase functions are forward-peaked, derived from Mie theory's infinite series solution involving spherical . These parameters enable simulations, with basic derivations stemming from the equation where the source function includes scattering integrals over p(θ).

Refraction

Refraction in the atmosphere occurs when rays bend to changes in the of air, which varies with and temperature. The nn of air is primarily determined by its , decreasing as altitude increases because air becomes less . This bending follows , expressed as n1sinθ1=n2sinθ2n_1 \sin \theta_1 = n_2 \sin \theta_2, where n1n_1 and n2n_2 are the of two adjacent air layers, and θ1\theta_1 and θ2\theta_2 are the angles of incidence and refraction, respectively. In the atmosphere, these layers create a , causing continuous deviation rather than discrete bends at interfaces. For gradual changes in refractive index with height hh, known as gradient refraction, light rays follow curved paths. The radius of curvature RR of such a ray path approximates RndndhR \approx -\frac{n}{\frac{dn}{dh}}, where the negative sign indicates downward curvature in a standard decreasing density profile. This formula arises from the differential form of applied to small vertical increments, accounting for how temperature lapse rates influence dndh\frac{dn}{dh}; a typical dry adiabatic lapse rate of about 9.8 K/km leads to a refractive index gradient that curves rays concave toward the . In a standard atmosphere, this results in rays bending with a radius on the order of 7-8 times the Earth's radius, effectively making the visual horizon appear farther. A key measure is the standard atmospheric refraction near the horizon, which elevates the apparent position of celestial objects by approximately 0.57 degrees (or 34 arcminutes), allowing the Sun to be visible about 2 minutes before it geometrically rises. This value assumes a standard profile and decreases with higher altitudes above the horizon. Diurnal variations in refraction arise from daily cycles, with values often higher due to cooler surface air creating steeper gradients, leading to greater bending; observations show average morning refractivity exceeding afternoon levels by up to 10-20 units in the modified refractive index. These effects significantly impact celestial observations, requiring corrections in astronomy to determine true positions of and , as uncorrected can introduce errors of several arcminutes in alt-azimuth measurements. Abnormal temperature gradients can produce looming (elevated apparent height of distant objects), sinking (lowered appearance), and towering (stretched vertical distortion) effects. occurs when an inversion layer increases the gradient, bending rays more sharply upward and making objects like ships or islands seem raised above the horizon. Sinking results from the opposite, a superadiabatic that curves rays downward more than usual, compressing the view. Towering combines elevation with elongation, often seen over water with subtle inversions, altering the perceived shape without inverting the image. These phenomena highlight how deviations from the standard modify ray paths, influencing and .

Reflection and Diffraction

Reflection in atmospheric optics follows the law of reflection, which states that the incident ray, the reflected ray, and the normal to the surface at the point of incidence all lie in the same plane, with the angle of incidence equal to the angle of reflection. This principle governs from smooth surfaces, such as calm water bodies producing sun glints or flat facets of ice crystals causing sparkling on surfaces. In the atmosphere, these reflections contribute to visible effects like vertical sun pillars formed by light bouncing off the horizontal facets of falling plate-like ice crystals. Total internal reflection occurs when light traveling within a medium of higher refractive index, such as water or ice, strikes the boundary with air at an angle greater than the critical angle, resulting in complete reflection back into the medium without transmission. The critical angle is determined by Snell's law and depends on the refractive indices of the media; for water-air interfaces, it is approximately 48.6 degrees. In atmospheric contexts, this phenomenon is essential for light paths inside water droplets and ice crystals, where it enables internal bounces that shape various optical displays, often in combination with refraction. Diffraction in atmospheric optics arises from the wave nature of interacting with small obstacles or comparable to the , leading to bending and interference patterns. The Huygens-Fresnel principle explains this as every point on a serving as a source of secondary spherical wavelets that interfere to form the field. For a circular , the far-field pattern manifests as an —a central bright spot surrounded by concentric rings—limiting the resolution of images formed by atmospheric particles. The approximate angular size of the first minimum in the Airy pattern, or angle, is given by θλ/d\theta \approx \lambda / d, where λ\lambda is the and dd is the diameter, highlighting how smaller particles produce wider spreads. In multiple scattering environments, such as hazy or cloudy atmospheres, reflection and interplay to distribute light through repeated interactions, altering intensity and direction without net absorption. Reflection from atmospheric surfaces also induces polarization effects; at (where the reflected and refracted rays are perpendicular), the reflected light becomes fully polarized perpendicular to the , influencing the observed polarization of skylight and glints. For water droplets, reflectivity varies with incidence angle, remaining low (around 2% at normal incidence) but increasing toward grazing angles due to the , which describe the partial reflection at interfaces. Ice crystal facets, often hexagonal and planar, enhance similar to mirrors, with their high reflectivity (up to near 100% for total internal cases) contributing to bright, localized atmospheric features.

Color Phenomena

Sky and Horizon Coloration

The coloration of the daytime sky arises primarily from Rayleigh scattering, where sunlight interacts with air molecules, preferentially scattering shorter blue wavelengths over longer red ones. This process results in the familiar blue hue observed overhead, as the scattering efficiency is inversely proportional to the fourth power of the wavelength, making blue light (around 450 nm) scatter about 4.4 times more effectively than red light (around 650 nm). Near the zenith, where the solar zenith angle is small, the sky appears a deeper blue due to the shorter optical path length through the atmosphere. As the approaches the horizon, the increases, leading to greater and thus brighter sky intensity. The relative τ along this path approximates τ ≈ 1 / cos z, where z is the angle, causing the to brighten significantly toward the horizon—often by a factor of 10 or more compared to the under clear conditions. This enhanced also shifts the color slightly toward paler blues and whites due to the inclusion of more forward-scattered light. Additionally, the exhibits strong from , reaching a maximum degree of polarization (up to 80-90%) at points 90° from the sun, with the vector oriented perpendicular to the sun-observer plane; this pattern aids in some animals but is imperceptible to most humans without aids. Around the sun itself, a brighter region known as the aureole forms due to by larger particles, which forward-scatters light more efficiently, creating a hazy halo that dims the blue Rayleigh background. During twilight, as the sun dips below the horizon, the increased atmospheric path length scatters out even more blue and green light from the direct beam, leaving predominantly red and orange hues to illuminate the sky and horizon. This effect intensifies with solar depression angles greater than 6°, producing vivid sunsets where the sky transitions from yellows to deep reds over distances equivalent to 20-40 times the vertical atmospheric thickness. A notable phenomenon in some clear twilights is the "purple light," a rosy-purple glow above the darker shadow of Earth, caused by the transmission of red light through a high-altitude ozone layer that selectively absorbs green and yellow wavelengths around 600 nm, combined with Rayleigh scattering of the remaining spectrum. Volcanic eruptions can dramatically enhance these red and purple tones by injecting sulfur aerosols into the stratosphere, which increase multiple scattering and absorption of shorter wavelengths; for instance, the 1815 eruption of Mount Tambora produced exceptionally fiery red sunsets and hazy purple skies across Europe and North America for over a year, contributing to the atmospheric conditions of the "year without a summer."

Cloud Coloration

Clouds typically appear white due to by water droplets approximately 10 micrometers in diameter, which scatters all visible wavelengths roughly equally, preventing significant color separation. This uniform scattering dominates in typical water clouds, where droplet sizes are comparable to visible light wavelengths, resulting in a bright, neutral appearance without preferential wavelength attenuation. Iridescence in clouds arises from diffraction of light by small, nearly uniform water droplets or ice crystals in thin cloud layers or at their edges, producing overlapping colored bands or patches. These colors emerge when droplet sizes vary gradually across the , causing shifts in diffraction angles that separate wavelengths. Such effects are most vivid in altocumulus or cirrus clouds near the sun or , displaying pastel hues like pink, green, and blue. Noctilucent clouds, occurring at high altitudes around 80 kilometers, exhibit a silvery-blue sheen from by tiny crystals illuminated by the sun below the horizon. can induce graying in clouds through absorbing aerosols like , which reduce by absorbing light within cloud layers, contrasting with the whitening effect of aerosols. In 2023, and ground observations documented notable iridescent displays, including early polar stratospheric clouds over showing vivid colors from particle . Notable iridescent displays continued in 2024 and 2025, including observations over in July 2025. At cloud edges, can serve as precursors to glories, where small-scale droplet uniformity produces faint rainbow-like rings around the observer's shadow. Coronas, concentric colored rings around the moon viewed through thin clouds, result from by similar small droplets, with ring size inversely proportional to droplet diameter and colors fading outward from white to violet innermost.

Size and Position Effects

Apparent Size of Sun and Moon

The refers to the common perceptual phenomenon where the Moon appears significantly larger when near the horizon than when high in the sky, despite its actual remaining nearly constant at approximately 0.5 degrees. This effect arises primarily from cognitive factors, including the brain's interpretation of relative distances and surrounding visual cues, such as terrestrial features that make the horizon Moon seem farther away, leading to an overestimation of its size via size-distance invariance. contributes minimally, actually compressing the Moon's vertical dimension slightly and making its apparent size about 1-2% smaller near the horizon due to the Moon being roughly 1.5% farther from the observer at that position. The illusion has been documented since antiquity, with the second-century astronomer Ptolemy providing one of the earliest descriptions in his Almagest, where he attributed the enlarged appearance to atmospheric refraction bending light rays through denser air layers near the horizon. In his later Optics, Ptolemy offered an alternative perceptual explanation involving the visual system's difficulty in judging angles at low elevations, highlighting the blend of optical and cognitive elements even in early accounts. There is no physical enlargement of the Moon's angular size; instead, experiments confirm a strong perceptual bias, as demonstrated in the 1940s studies by Holway and Boring, who used artificial moons projected at varying elevations and found that perceived size decreased systematically with the angle of regard, independent of actual distance cues. This perceptual bias is culturally notable in phenomena like the harvest moon, the full moon closest to the autumnal equinox, which often rises near the horizon during harvest season and appears dramatically enlarged against the landscape, inspiring folklore and art across many societies. The Sun exhibits a related effect known as flattening or ellipticity near the horizon, where its disk appears compressed vertically into an oval shape due to differential atmospheric refraction, which bends rays from the lower limb more than those from the upper limb. The Sun's true angular diameter is about 0.5 degrees, but this refraction reduces the vertical extent by roughly 15-20% at the horizon, creating an asymmetry of around 5-9 arcminutes across the disk. Like the Moon, there is no actual change in the Sun's physical size; the distortion is purely optical, enabled by the gradient in atmospheric density, and simulations of refraction effects confirm the minor 1-2% overall impact on apparent dimensions.

Atmospheric Refraction

Atmospheric refraction causes light from celestial bodies to bend as it passes through layers of air with varying densities, primarily due to and gradients, resulting in an apparent of objects near the horizon. Atmospheric refraction near the horizon displaces the apparent position of stars and the Sun upward by approximately 35 arcminutes under standard conditions. For the Sun, this makes it appear above the geometric horizon when its is actually below it, leading to sunrise occurring about 2 minutes earlier and sunset about 2 minutes later than without atmospheric effects, with variations depending on and —typically around 1 minute at low latitudes and several minutes at higher ones. A prominent phenomenon arising from this is the , observed at sunset (or sunrise) when the Sun's upper rim briefly appears due to chromatic dispersion, where shorter wavelengths like green are refracted more than longer ones like red. This occurs as the last visible part of the Sun crosses the horizon, with the green segment lasting approximately 1-2 seconds under clear conditions with a stable atmospheric layer. Historical measurements of , such as those conducted by François Arago and in the early 19th century, provided foundational data on the of air, estimating its value through astronomical observations and establishing that it varies minimally from for dry air, enabling more precise models of light bending. In modern contexts, alterations in atmospheric lapse rates—potentially influenced by —may enhance conditions for green flashes by stabilizing inversion layers, though direct increases in frequency remain under study. Related effects include the twilight arch, where the apparent rise of forms a colored band opposite the setting Sun, and rare purple flashes, which can appear when aerosols selectively absorb or scatter green light, modifying the dispersion spectrum.

Ice Crystal Phenomena

Halos

Halos are optical phenomena appearing as circular rings of light encircling the Sun or Moon, primarily caused by the refraction of sunlight through ice crystals suspended in high-altitude cirrus or cirrostratus clouds. These crystals, typically hexagonal in structure, act as prisms that bend incoming rays, concentrating light at specific angular distances from the light source. The most common halos form when the crystals are randomly oriented, leading to a symmetric ring visible to observers on the ground. The , the most frequently observed type, results from through the 60° prism faces of hexagonal plate-shaped crystals. Sunlight enters one face, refracts inside the crystal with n ≈ 1.31 for , and exits the adjacent face, producing a angle of approximately 22°. This δ is given by δ = 2(i - r), where i is the angle of incidence and r = arcsin(sin i / n) is the angle of ; the minimum occurs for symmetric passage through the prism, yielding δ ≈ 21.8° for . Due to dispersion, red light (n ≈ 1.306) deviates less (≈ 21.5°), forming a sharp red inner edge, while blue light (n ≈ 1.317) deviates more (≈ 22.4°), creating a diffuse outer edge with subtle coloration. The rarer 46° halo arises from in hexagonal column-shaped ice crystals, where sunlight enters a prism side face and exits through a basal (end) face, resulting in a larger of about 46°. This configuration requires precise alignment and is less common because randomly oriented columns produce a fainter ring compared to the efficient 60° prisms of plates; pristine, undistorted crystals are essential for visibility, often appearing through thin cirrostratus clouds. Variations such as and the occur when ice crystals align their c-axes horizontally or vertically due to aerodynamic forces. arcs form as bright extensions touching the top or bottom of the from plate crystals with horizontal c-axes, merging into a circumscribed halo when the Sun is higher. The , an upside-down rainbow-like band, results from vertical c-axis plate crystals refracting light through their upper and lower faces at near-minimum deviation. These features were first systematically explained by in his 1637 work Les Météores, attributing halos to in elongated ice particles rather than earlier mythological interpretations.

Sun Dogs

Sun dogs, also known as parhelia, are bright, localized spots of light that appear approximately 22° to the left and right of the Sun at the same elevation above the horizon, resulting from the of through atmospheric ice crystals. These phenomena are distinct from full halo rings, serving as prominent bright patches within or alongside them. They occur when horizontally oriented, plate-shaped hexagonal ice crystals—typically found in high-altitude cirrus or cirrostratus clouds—refract incoming , with the light rays entering one side face and exiting another at a angle of 22°. This is most pronounced when the Sun is low in the sky, as higher positions can reduce the prominence of the spots due to the of the crystals. The appearance of sun dogs resembles mock suns, often displaying subtle colors from dispersion, where shorter wavelengths are refracted more than longer red ones, creating a with red nearest the Sun and fading to yellow, orange, and outward; the ice crystals effectively act as 60° prisms. In favorable conditions, these spots develop luminous tails extending horizontally along the parhelic circle—a faint band of light at the Sun's altitude formed by reflections off the vertical faces of the crystals—which can stretch across much of the sky and enhance the mock-sun effect. Sun dogs are most frequent in cold climates, where abundant ice crystals in cirrus clouds or near-ground provide ideal conditions for their formation. The name "sun dog" derives from early observations of these spots trailing the Sun across the sky, akin to a dog following its master, with the term in use since at least the . In environments rich with —tiny ice crystals suspended near the surface in polar or subpolar regions—sun dogs can manifest as elongated bright segments or even full circles along the parhelic circle, offering striking observations during clear, frigid weather.

Dispersion and Reflection Effects

Rainbows

Rainbows form through the interaction of with spherical water droplets in the atmosphere, primarily via , internal reflection, and dispersion of light. In the primary rainbow, enters a droplet, undergoes a single internal reflection off the inner surface, and exits after further , with the resulting rays concentrated around a angle that produces a bright arc. This process separates white light into its spectral colors due to the varying refractive indices for different wavelengths, creating a sequence from on the outer edge to violet on the inner edge. Ray tracing through idealized spherical droplets reveals that light deviates by approximately 138°, corresponding to an angular radius of 42° from the , while violet light deviates more sharply to yield a 40° radius, causing the color banding. The secondary rainbow arises from rays undergoing two internal reflections within the droplet before exiting, leading to greater overall deviation and a fainter arc positioned outside the primary one. This double reflection reverses the color order, with violet appearing on the outer edge and on the inner, and positions the bow at a radius of about 51° for . Between the primary and secondary rainbows lies Alexander's dark band, a noticeably dimmer region where raindrops do not deviate toward the observer, as rays from those angles are scattered elsewhere—either inside the primary arc or outside the secondary. Fogbows, or white rainbows, occur with very small droplets (typically under 0.05 mm in diameter) in or , where dominates over , causing spectral colors to overlap and produce a pale, nearly colorless arc larger than a standard . Lunar rainbows, known as moonbows, form similarly but under moonlight, appearing faint and often white to the due to the moon's lower intensity, though colors may be discernible in long-exposure photographs. In the , advanced the understanding of colors in his Opticks (1704), demonstrating through prism experiments that white light decomposes into a continuous of colors, with the rainbow's hues resulting from differential rather than modification of light. Supernumerary bands, faint additional arcs inside the primary rainbow, emerge prominently with uniform small droplets (around 0.5–1 mm), where between multiple ray paths enhances specific wavelengths. George Biddell Airy's 1838 approximated this interference using a differential approach to the ray deviation angle near the rainbow's caustic, predicting the bands' spacing and intensity as functions of droplet size, thus bridging with wave .

Glories

A glory is an characterized by a series of brightly colored, concentric rings surrounding the shadow of the observer, formed by the backscattering of from small, uniform droplets in clouds or . This effect occurs when light rays interact with spherical droplets, typically 4 to 25 micrometers in radius, undergoing multiple internal reflections and diffractions that result in constructive interference at specific angles. The phenomenon is explained through theory, which accurately predicts the glory's appearance for spherical particles, with the rings arising from interference between surface waves that propagate around the droplet's circumference. The angular radius of a glory's rings typically spans 5 to 20 degrees from the , with the innermost red ring appearing at smaller angles for larger droplets and expanding outward to form multiple, successively dimmer colored bands due to higher-order interference. These rings exhibit a similar to but in reverse, with red on the outer edges and blue-violet toward the center, though the glory's backscattered nature distinguishes it from forward-scattered rainbow arcs. The glory requires a layer of uniform droplets opposite the sun from the observer, often visible from or mountaintops, and its visibility depends on the narrow size distribution of the droplets, as polydispersity broadens and fades the rings. When the observer's enlarged shadow is cast on a cloud deck, encircles it, creating the , a dramatic sight historically linked to eerie and supernatural perceptions in and . In aviation, pilots often encounter this as a "pilot's glory" or around the aircraft's shadow, serving as an indicator of in clouds below, which can signal potential icing risks. Mountain observations are common, such as from ridges above layers, where the effect's scale amplifies its striking presence. Recent 2024 analyses of , including MODIS data, have demonstrated that spectral differences in glories directly reflect cloud droplet size distributions, confirming links to small, uniform droplets in the upper cloud layers and enabling of microphysical properties. The glory's rings display a high degree of , predominantly radial (positive) in the colored portions, with parallel polarization dominating over , which contributes to its ethereal quality and aids in distinguishing it from other aureoles. This polarization arises from the coherent backscattering geometry, enhancing contrast in polarized light observations and providing additional diagnostic tools for droplet characterization.

Mirage Effects

Inferior and Superior Mirages

Mirages are optical phenomena arising from the refraction of light through atmospheric layers with varying temperatures, which alter the refractive index and cause light rays to bend along curved paths that minimize travel time according to Fermat's principle. This principle states that light follows the path of stationary optical length, equivalent to least time, where the speed of light in air varies as c=c0/nc = c_0 / n, with c0c_0 being the vacuum speed and nn the refractive index decreasing with temperature. Inferior and superior mirages represent the basic forms, distinguished by the direction of ray curvature due to surface temperature inversions. Inferior mirages occur under conditions of a hot surface creating a inversion, where warm air lies beneath cooler air aloft, producing a strong near the ground./22:_Atmospheric_Optics/22.6:_Mirages) This , often exceeding 10°C/km on average but reaching 10–20°C over just a few centimeters in extreme cases, decreases the air density and with height, causing light rays from distant objects to curve upward away from the hotter layer./22:_Atmospheric_Optics/22.6:_Mirages) As a result, an inverted, oscillating image appears below the actual object, mimicking a reflection as if from a watery surface; a classic example is the "puddle" on hot sands or asphalt roads, where the sky seems mirrored below the horizon. These effects are enhanced by in the unstable warm-under-cold air, leading to shimmering distortions./22:_Atmospheric_Optics/22.6:_Mirages) Superior mirages, in contrast, form over cold surfaces such as or , where a temperature inversion places colder air below warmer air, creating a positive that bends rays downward toward the denser lower layer. This elevates and distorts the apparent position of objects, producing effects where distant features appear taller or suspended above the horizon, often with an inverted image stacked above the erect one. A representative example is the sight of ships appearing to float ethereally over the sea, their hulls hidden while masts unnaturally high. Such mirages require inversions of at least a few degrees over tens of meters and are prevalent in stable stratified conditions./22:_Atmospheric_Optics/22.6:_Mirages) These simple superior mirages served as both aids and deceptions in 19th-century Arctic explorations, where observers like in 1820 reported inverted ships and elevated landmasses that confounded distance estimates and navigation. Complex variants, such as the Fata Morgana, build on these by involving multiple inversions for layered distortions.

Fata Morgana and Novaya Zemlya Effect

The Fata Morgana is a complex form of superior that produces multiple, distorted, and rapidly fluctuating images of distant objects, often appearing as towering, elongated structures or inverted layers stacked above the horizon. This phenomenon arises from strong temperature inversions in the atmosphere, where layers of warmer air overlie cooler air near the surface, creating gradients in that cause light rays to undergo repeated total internal reflections and ducting within stable air masses. Such conditions trap and bend light rays in a way that extends the visibility of objects over water or land, resulting in compressed, stretched, and alternating erect and inverted images. Historically associated with myths of illusory cities or castles, the Fata Morgana is frequently observed in regions like the , where stable atmospheric layers over the sea enhance the ducting effect and produce dramatic, multi-layered distortions of coastlines or ships. Ray-tracing simulations of these events, incorporating spherically non-symmetric atmospheric models with multiple inversion layers, accurately reproduce the observed striations and elongations by tracing light paths through varying gradients. For instance, simulations using parameters such as a ground temperature of -30°C and inversion heights up to 80 m demonstrate how ducting creates "wall-like" illusions of distant features. The effect represents another manifestation of superior mirage ducting, particularly in polar regions, where it bends the image of the Sun or well above the geometric horizon, allowing its visibility during periods of extended . This occurs through within a strong, horizontally extensive inversion layer, or , that acts as a light duct, curving rays with a radius tighter than the Earth's surface and effectively advancing sunrise or delaying sunset by several days. The phenomenon was first documented during Willem Barentsz's 1596–1597 expedition, when crew member Gerrit de Veer recorded sightings of a mock Sun on January 24 and 27, 1597. On these dates, the true solar altitude was approximately -5.4° and -4.7° below the horizon, respectively, yet the mock Sun appeared above the horizon. Ray-tracing models of the effect, applied to historical accounts like de Veer's, confirm that a single strong inversion or multiple weaker ones can trap solar rays over distances exceeding 200 km, producing elongated or striped solar images that evolve over days as the inversion persists. These simulations, using flat or curved approximations with differentials of 1–8°C across inversion heights of 13–80 m, match observed timings and distortions, such as the Sun appearing as horizontal bands during Fridtjof Nansen's expedition. Both the Fata Morgana and effect highlight the role of atmospheric ducting in extending basic superior mirages into multi-layered optical illusions, reliant on prolonged stability in inversion layers for their persistence.

Ray and Shadow Phenomena

Crepuscular Rays

, also known as sunbeams or god rays, are visible shafts of that appear to radiate from the position of the low sun, typically during sunrise or sunset, when light streams through gaps in clouds or other obstacles. These rays are most prominent when the sun is near the horizon, creating dramatic beams separated by shadowed regions cast by the clouds. The phenomenon is caused by the of by atmospheric particles such as , aerosols, droplets, or air molecules, which makes the otherwise invisible beams discernible against the darker shadows. The formation of crepuscular rays occurs when parallel rays of from the distant sun pass through irregular gaps in a layer of clouds, mountains, or forests, with the being selectively scattered forward by particles in the atmosphere while shadowed areas block the . This selective transmission highlights the illuminated columns of air, and the rays become more visible in hazy conditions where larger particles enhance , providing sufficient brightness contrast. The low solar elevation angle during crepuscular periods (twilight) elongates the path through the atmosphere, increasing scattering opportunities and thus ray visibility. Laboratory simulations confirm that ray intensity peaks due to multiple small-angle forward before exponential decay from extinction, with colors ranging from white in turbid air to bluish in cleaner atmospheres. In appearance, crepuscular rays project forward from the sun, often emerging from low-altitude clouds and fanning outward in a converging toward the observer, with occasional color gradients along the beams due to wavelength-dependent —shorter wavelengths scattering more than . The rays can span vast distances, illuminating landscapes or sea surfaces, and are enhanced by high humidity or that boosts particle density for brighter beams. These rays are commonly observed in temperate regions during clear-to-partly cloudy evenings, creating a striking interplay of and shadow that has inspired awe in observers. Key facts about include their enhanced visibility in hazy atmospheres, where dust or smoke scatters light effectively without excessive absorption, and their extension across the sky to the , where they may appear as . Historically, depictions of appear in , such as in landscape paintings by artists like and , symbolizing divine intervention or natural grandeur, though they were rarely shown in medieval works before becoming more common in the 15th and 16th centuries. Optically, crepuscular rays exhibit no actual or convergence; the parallel sunbeams only appear to fan out due to linear perspective, similar to how parallel railroad tracks seem to meet at a on the horizon. This arises because the observer's viewpoint compresses the distant parallel rays into converging lines, with the sun serving as the apparent origin point. Simulations of natural scenes, such as rays through rectangular gaps, demonstrate that the perceived angle depends on the observer's position relative to the layer and medium.

Anticrepuscular Rays and Belt of Venus

Anticrepuscular rays, also known as antisolar rays, are beams of sunlight that appear to converge toward the on the horizon opposite the Sun, typically visible during or . These rays form as extensions of , where shadows cast by clouds or mountains scatter light through gaps, but observers see the effect in the opposite direction due to the of the . Although they seem to meet at a , the rays are actually parallel, with the apparent convergence resulting from a perspective similar to parallel railroad tracks appearing to join in the distance. This highlights the role of linear perspective in atmospheric optics, where the of the and the observer's viewpoint create the deceptive narrowing. The , or antitwilight arch, is a pinkish-purple band that appears as a diffuse arc spanning the sky opposite the setting or rising Sun, just above the dark silhouette of on the horizon. This glow arises from of in the upper atmosphere, where shorter wavelengths are scattered away, leaving longer red and pink hues to backlight aerosols and air molecules in the denser lower . The band marks the boundary between the illuminated upper atmosphere and the encroaching shadow cone of , which extends into as an umbra during twilight, casting a triangular dark zone below the arch. Visibility is enhanced under clear skies with minimal low-altitude haze, as the effect relies on backscattering of reddened from the horizon. Together, and the illustrate the interplay of shadow projection and scattering in the evening sky, with rays often piercing through the arch for striking contrasts. The phenomena are most prominent when the Sun is low, allowing the to align near the horizon and maximizing the shadow's ascent.

Diffraction Phenomena

Coronas

A corona is an characterized by a series of faintly colored concentric rings surrounding a bright light source, such as the Sun or , produced by the of through small, uniformly sized particles in the atmosphere. These aureoles form primarily when or moonlight encounters clouds composed of droplets typically 1–20 micrometers in , such as in altocumulus or cirrocumulus formations, where the particles act as obstacles causing diffracted waves to interfere constructively and destructively. The central region appears as a bright white disk, transitioning outward to colored fringes where the first ring exhibits blue-violet on the inner edge grading to red on the outer edge, with subsequent rings showing muted greens, yellows, and reds due to overlapping patterns. The angular radius θ of the primary corona ring is approximated by θ ≈ 1.22 λ / d, where λ is the of and d is the droplet , allowing the of the particles to be estimated from observed ring spacing—for instance, droplets around 10 μm produce rings with radii of about 5–10 degrees. Coronas often appear around the Moon in thin cirrus clouds, creating ethereal displays visible to the under clear night skies. Historical observations highlight how aerosols and particles in the can generate similar but more diffuse effects. A prominent variant is , a broader corona with a radius of approximately 15–20 degrees, featuring a pale blue inner aureole edged in reddish-brown, formed by from larger particles (around 1–2 μm) lofted into the upper atmosphere, as notably observed after the 1883 eruption. These rings lack the vivid colors of standard due to the particles' absorbing properties but still arise from the same principles. Polarization patterns in coronas reveal the diffraction process, with measurements showing partial tangential to the rings, enabling of cloud microphysics via techniques. By analyzing ring dimensions and colors, scientists can infer droplet sizes and uniformity, providing insights into cloud composition without direct sampling.

Atmospheric Diffraction Overview

Atmospheric diffraction refers to the bending and spreading of waves as they interact with atmospheric structures and particles, distinct from or , and plays a crucial role in various optical phenomena beyond the well-known coronas around celestial bodies. In the context of wave optics, occurs when encounters edges or apertures comparable to its , leading to interference patterns that alter through the atmosphere. This process is governed by principles such as the Huygens-Fresnel principle, where secondary wavelets from wavefronts interfere constructively or destructively. Applications of these wave optics concepts in atmospheric studies emerged prominently in the , particularly in modeling for and visibility assessments, building on foundational work by in the early 1800s but extended through computational advancements in the mid-1900s. Edge diffraction in the atmosphere manifests as the bending of around obstacles, such as ridges or terrain features, where the first —a cylindrical region around the line-of-sight path with radius proportional to the of the distance—determines whether diffraction losses occur. If the obstacle encroaches into this zone, waves around the edge, creating a shadow region with gradual illumination rather than a sharp boundary, analogous to knife-edge diffraction models used in wave . This effect is particularly relevant in predictions over irregular terrain, where the parameter quantifies the depth of the receiver into the shadow, influencing signal or intensity beyond the geometric horizon. Recent analyses of losses in hilly regions highlight how clearance affects , with applications extending from radio waves to visible in atmospheric optics. In hazy or foggy conditions, diffraction contributes to forward aureoles—bright rings or glows around sources—arising from the forward of by large particles, where dominates over other mechanisms for particles much larger than the . These aureoles reduce contrast in the forward direction, extending Koschmieder's law, which relates to atmospheric extinction coefficient (typically V=3.91βV = \frac{3.91}{\beta}, where β\beta is the extinction coefficient), by accounting for the enhanced forward transmission that masks distant objects. Empirical models incorporating aureole effects show that size distributions and concentrations directly influence aureole brightness and extent, impacting estimates in polluted or dusty atmospheres. propagation analogies further illustrate this, as over terrain in microwave bands mirrors optical haze effects, with both relying on Fresnel-Kirchhoff integrals for loss calculations. Atmospheric turbulence induces diffraction through small-scale refractive index fluctuations, contributing to phenomena like the twinkling or scintillation of stars, where distortions create intensity variations via interference of diffracted paths. This scintillation arises from the modulation of light amplitude and phase, with the variance in log-intensity given by expressions involving the turbulence strength parameter Cn2C_n^2 and path length, emphasizing 's role alongside . These insights underscore 's broader impact on atmospheric wave propagation, from visibility to .

Historical Development

Early Observations and Theories

Early observations of atmospheric optics date back to ancient civilizations, where natural phenomena like rainbows and halos were often interpreted through philosophical and mythological lenses. In the 4th century BCE, proposed in his Meteorologica that rainbows arise from the reflection of sunlight off clouds at a fixed angle, viewing them as a form of solar reflection rather than through water droplets. This qualitative explanation integrated rainbows into broader meteorological theories but lacked empirical testing. Similarly, in the , the Persian scholar (Alhazen) advanced understanding of light propagation in his seminal (1021 CE), providing the first accurate description of as light bends when passing from one medium to another, such as air to water; this laid essential groundwork for explaining atmospheric bending effects like mirages and halos. During the medieval period, European and Islamic scholars built on these foundations through experimentation and detailed descriptions. In the 13th century, English friar conducted pioneering experiments on rainbows, using prisms and water-filled globes to demonstrate that colors result from and reflection within spherical droplets, emphasizing the role of observer position at approximately 42 degrees from the ; his work in (1267) highlighted the value of empirical verification in . Cultural interpretations often wove these phenomena into myths, reflecting pre-scientific attempts to explain the unfamiliar. The advent of the in the early , invented around 1608 by Hans Lippershey and refined by , enhanced observations of celestial bodies but also indirectly illuminated atmospheric optics by revealing distortions from , such as in measurements of stellar positions. A key milestone came in 1637 with ' Les Météores, appended to his Discours de la méthode, where he mathematically derived the rainbow's angular laws using geometric : primary rainbows form via one internal reflection in raindrops at 42 degrees, and secondary at 51 degrees, based on of (though Descartes formulated his own version). This mechanistic approach shifted atmospheric optics toward quantitative physics, influencing subsequent research.

Modern Advances and Research

In the 19th century, significant theoretical advancements in atmospheric optics laid the groundwork for understanding light scattering and interference phenomena. George Biddell Airy developed a mathematical model in the 1830s incorporating wave interference to explain the intensity distribution near rainbow caustics, resolving the infinite intensity paradox predicted by earlier ray optics approaches by showing that interference fringes limit the brightness at the rainbow edge. This work, published in 1838, marked a pivotal shift toward wave-based explanations in optics. Complementing this, Lord Rayleigh derived the scattering formula for small particles in 1871, demonstrating that the scattered intensity I is proportional to 1/λ⁴, where λ is the wavelength, thus explaining the blue color of the sky as shorter wavelengths are preferentially scattered by atmospheric molecules. The 20th century saw further refinements, particularly with Gustav Mie's comprehensive theory in 1908, which extended electromagnetic scattering solutions to spherical particles of arbitrary size using , enabling accurate predictions for light interaction with aerosols and cloud droplets beyond the Rayleigh limit. Computational simulations emerged in the 1970s and 1980s, with early programs modeling halo formations by tracing rays through orientations, as detailed in Robert Greenler's 1980 work on ray paths in hexagonal prisms, which simulated complex displays like sundogs and 22° halos. NASA's contributions, including satellite-based measurements from instruments like MODIS since the early 2000s, have quantified aerosol and its radiative effects, aiding in global climate modeling by linking to atmospheric composition. Recent data from NASA's PACE mission, launched in February 2024, continue to advance of aerosols and ocean ecosystems, providing insights into atmospheric optics as of 2025.

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