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Solar eclipse
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A total solar eclipse occurs when the Moon completely covers the Sun's disk. Solar prominences can be seen along the limb (in red) as well as extensively the coronal and partly the radiating coronal streamers. (August 11, 1999) | |
An annular solar eclipse occurs when the Moon is too far away to completely cover the Sun's disk (October 14, 2023). | |
During a partial solar eclipse, the Moon blocks only part of the Sun's disk (October 25, 2022). |
A solar eclipse occurs when the Moon passes between Earth and the Sun, thereby obscuring the view of the Sun from a small part of Earth, totally or partially. Such an alignment occurs approximately every six months, during the eclipse season in its new moon phase, when the Moon's orbital plane is closest to the plane of Earth's orbit.[1] In a total eclipse, the disk of the Sun is fully obscured by the Moon. In partial and annular eclipses, only part of the Sun is obscured. Unlike a lunar eclipse, which may be viewed from anywhere on the night side of Earth, a solar eclipse can only be viewed from a relatively small area of the world. As such, although total solar eclipses occur somewhere on Earth every 18 months on average, they recur at any given place only once every 360 to 410 years.
If the Moon were in a perfectly circular orbit and in the same orbital plane as Earth, there would be total solar eclipses at every new moon. Instead, because the Moon's orbit is tilted at about 5 degrees to Earth's orbit, its shadow usually misses Earth. Solar (and lunar) eclipses therefore happen only during eclipse seasons, resulting in at least two, and up to five, solar eclipses each year, no more than two of which can be total.[2][3] Total eclipses are rarer because they require a more precise alignment between the centers of the Sun and Moon, and because the Moon's apparent size in the sky is sometimes too small to fully cover the Sun.
An eclipse is a natural phenomenon. In some ancient and modern cultures, solar eclipses were attributed to supernatural causes or regarded as bad omens. Astronomers' predictions of eclipses began in China as early as the 4th century BC; eclipses hundreds of years into the future may now be predicted with high accuracy.
Looking directly at the Sun can lead to permanent eye damage, so special eye protection or indirect viewing techniques are used when viewing a solar eclipse. Only the total phase of a total solar eclipse is safe to view without protection. Enthusiasts known as eclipse chasers or umbraphiles travel to remote locations to see solar eclipses.[4][5]
Predictions
[edit]Geometry
[edit]
The diagrams to the right show the alignment of the Sun, Moon, and Earth during a solar eclipse. The dark gray region between the Moon and Earth is the umbra, where the Sun is completely obscured by the Moon. The small area where the umbra touches Earth's surface is where a total eclipse can be seen. The larger light gray area is the penumbra, in which a partial eclipse can be seen. An observer in the antumbra, the area of shadow beyond the umbra, will see an annular eclipse.[6]
The Moon's orbit around Earth is inclined at an angle of just over 5 degrees to the plane of Earth's orbit around the Sun (the ecliptic). Because of this, at the time of a new moon, the Moon will usually pass to the north or south of the Sun. A solar eclipse can occur only when a new moon occurs close to one of the points (known as nodes) where the Moon's orbit crosses the ecliptic.[7]
As noted above, the Moon's orbit is also elliptical. The Moon's distance from Earth varies by up to about 5.9% from its average value. Therefore, the Moon's apparent size varies with its distance from Earth, and it is this effect that leads to the difference between total and annular eclipses. The distance of Earth from the Sun also varies during the year, but this is a smaller effect (by up to about 0.85% from its average value). On average, the Moon appears to be slightly (2.1%) smaller than the Sun as seen from Earth, so the majority (about 60%) of central eclipses are annular. It is only when the Moon is closer to Earth than average (near its perigee) that a total eclipse occurs.[8][9]
| Moon | Sun | |||
|---|---|---|---|---|
| At perigee (nearest) |
At apogee (farthest) |
At perihelion (nearest) |
At aphelion (farthest) | |
| Mean radius | 1737.10 km (1079.38 mi) |
696000 km (432000 mi) | ||
| Distance | 363104 km (225622 mi) |
405696 km (252088 mi) |
147098070 km (91402500 mi) |
152097700 km (94509100 mi) |
| Angular diameter[10] |
33' 30" (0.5583°) |
29' 26" (0.4905°) |
32' 42" (0.5450°) |
31' 36" (0.5267°) |
| Apparent size to scale |
||||
| Order by decreasing apparent size |
1st | 4th | 2nd | 3rd |
The Moon orbits Earth in approximately 27.3 days, relative to a fixed frame of reference. This is known as the sidereal month. However, during one sidereal month, Earth has revolved part way around the Sun, making the average time between one new moon and the next longer than the sidereal month: it is approximately 29.5 days. This is known as the synodic month and corresponds to what is commonly called the lunar month.[7]
The Moon crosses from south to north of the ecliptic at its ascending node, and vice versa at its descending node.[7] However, the nodes of the Moon's orbit are gradually moving in a retrograde motion, due to the action of the Sun's gravity on the Moon's motion, and they make a complete circuit every 18.6 years. This regression means that the time between each passage of the Moon through the ascending node is slightly shorter than the sidereal month. This period is called the nodical or draconic month.[11]
Finally, the Moon's perigee is moving forwards or precessing in its orbit and makes a complete circuit in 8.85 years. The time between one perigee and the next is slightly longer than the sidereal month and known as the anomalistic month.[12]
The Moon's orbit intersects with the ecliptic at the two nodes that are 180 degrees apart. Therefore, the new moon occurs close to the nodes at two periods of the year approximately six months (173.3 days) apart, known as eclipse seasons, and there will always be at least one solar eclipse during these periods. Sometimes the new moon occurs close enough to a node during two consecutive months to eclipse the Sun on both occasions in two partial eclipses. This means that, in any given year, there will always be at least two solar eclipses, and there can be as many as five.[13]
Eclipses can occur only when the Sun is within about 15 to 18 degrees of a node, (10 to 12 degrees for central eclipses). This is referred to as an eclipse limit, and is given in ranges because the apparent sizes and speeds of the Sun and Moon vary throughout the year. In the time it takes for the Moon to return to a node (draconic month), the apparent position of the Sun has moved about 29 degrees, relative to the nodes.[2] Since the eclipse limit creates a window of opportunity of up to 36 degrees (24 degrees for central eclipses), it is possible for partial eclipses (or rarely a partial and a central eclipse) to occur in consecutive months.[14][15]
Path
[edit]
During a central eclipse, the Moon's umbra (or antumbra, in the case of an annular eclipse) moves rapidly from west to east across Earth. Earth is also rotating from west to east, at about 28 km/min at the Equator, but as the Moon is moving in the same direction as Earth's rotation at about 61 km/min, the umbra almost always appears to move in a roughly west–east direction across a map of Earth at the speed of the Moon's orbital velocity minus Earth's rotational velocity.[16]
The width of the track of a central eclipse varies according to the relative apparent diameters of the Sun and Moon. In the most favourable circumstances, when a total eclipse occurs very close to perigee, the track can be up to 267 km (166 mi) wide and the duration of totality may be over 7 minutes.[17] Outside of the central track, a partial eclipse is seen over a much larger area of Earth. Typically, the umbra is 100–160 km wide, while the penumbral diameter is in excess of 6400 km.[18]
Besselian elements are used to predict whether an eclipse will be partial, annular, or total (or annular/total), and what the eclipse circumstances will be at any given location.[19]: Chapter 11
Calculations with Besselian elements can determine the exact shape of the umbra's shadow on Earth's surface. But at what longitudes on Earth's surface the shadow will fall, is a function of Earth's rotation, and on how much that rotation has slowed down over time. A number called ΔT is used in eclipse prediction to take this slowing into account. As Earth slows, ΔT increases. ΔT for dates in the future can only be roughly estimated because Earth's rotation is slowing irregularly. This means that, although it is possible to predict that there will be a total eclipse on a certain date in the far future, it is not possible to predict in the far future exactly at what longitudes that eclipse will be total. Historical records of eclipses allow estimates of past values of ΔT and so of Earth's rotation. [19]: Equation 11.132
Duration
[edit]The following factors determine the duration of a total solar eclipse (in order of decreasing importance):[20][21]
- The Moon being almost exactly at perigee (making its angular diameter as large as possible).
- Earth being very near aphelion (furthest away from the Sun in its elliptical orbit, making its angular diameter nearly as small as possible).
- The midpoint of the eclipse being very close to Earth's equator, where the rotational velocity is greatest and is closest to the speed of the lunar shadow moving over Earth's surface.
- The vector of the eclipse path at the midpoint of the eclipse aligning with the vector of Earth's rotation (i.e. not diagonal but due east).
- The midpoint of the eclipse being near the subsolar point (the part of Earth closest to the Sun).
The longest eclipse that has been calculated thus far is the eclipse of July 16, 2186 (with a maximum duration of 7 minutes 29 seconds over northern Guyana).[20]
Types
[edit]
The Sun's distance from Earth is about 400 times the Moon's distance, and the Sun's diameter is about 400 times the Moon's diameter. Because these ratios are approximately the same, the Sun and the Moon as seen from Earth appear to be approximately the same size: about 0.5 degree of arc in angular measure.[22]
The Moon's orbit around Earth is slightly elliptical, as is Earth's orbit around the Sun. The apparent sizes of the Sun and Moon therefore vary.[23] The magnitude of an eclipse is the ratio of the apparent size of the Moon to the apparent size of the Sun during an eclipse. An eclipse that occurs when the Moon is near its closest distance to Earth (i.e., near its perigee) can be a total eclipse because the Moon will appear to be large enough to completely cover the Sun's bright disk or photosphere; a total eclipse has a magnitude greater than or equal to 1.000. Conversely, an eclipse that occurs when the Moon is near its farthest distance from Earth (i.e., near its apogee) can be only an annular eclipse because the Moon will appear to be slightly smaller than the Sun; the magnitude of an annular eclipse is less than 1.[24]
Because Earth's orbit around the Sun is also elliptical, Earth's distance from the Sun similarly varies throughout the year. This affects the apparent size of the Sun in the same way, but not as much as does the Moon's varying distance from Earth.[22] When Earth approaches its farthest distance from the Sun in early July, a total eclipse is somewhat more likely, whereas conditions favour an annular eclipse when Earth approaches its closest distance to the Sun in early January.[25]
There are three main types of solar eclipses:[26]
Total eclipse
[edit]A total eclipse occurs on average every 18 months[27] when the dark silhouette of the Moon completely obscures the bright light of the Sun, allowing the much fainter solar corona to be visible. During an eclipse, totality occurs only along a narrow track on the surface of Earth.[28] This narrow track is called the path of totality.[29]
Annular eclipse
[edit]An annular eclipse, like a total eclipse, occurs when the Sun and Moon are exactly in line with Earth. During an annular eclipse, however, the apparent size of the Moon is not large enough to completely block out the Sun.[22] Totality thus does not occur; the Sun instead appears as a very bright ring, or annulus, surrounding the dark disk of the Moon.[22] Annular eclipses occur once every one or two years, not annually.[27][30] The term derives from the Latin root word anulus, meaning "ring", rather than annus, for "year".[30]
Partial eclipse
[edit]A partial eclipse occurs about twice a year,[27] when the Sun and Moon are not exactly in line with Earth and the Moon only partially obscures the Sun. This phenomenon can usually be seen from a large part of Earth outside of the track of an annular or total eclipse. However, some eclipses can be seen only as a partial eclipse, because the umbra passes above Earth's polar regions and never intersects Earth's surface.[22] Partial eclipses are virtually unnoticeable in terms of the Sun's brightness, as it takes well over 90% coverage to notice any darkening at all. Even at 99%, it would be no darker than civil twilight.[31]

Hybrid eclipse
[edit]A hybrid eclipse (also called annular/total eclipse) shifts between a total and annular eclipse. At certain points on the surface of Earth, it appears as a total eclipse, whereas at other points it appears as annular. Hybrid eclipses are comparatively rare.[22]
A hybrid eclipse occurs when the magnitude of an eclipse changes during the event from less to greater than one, so the eclipse appears to be total at locations nearer the midpoint, and annular at other locations nearer the beginning and end, since the sides of Earth are slightly further away from the Moon. These eclipses are extremely narrow in their path width and relatively short in their duration at any point compared with fully total eclipses; the 2023 April 20 hybrid eclipse's totality is over a minute in duration at various points along the path of totality. Like a focal point, the width and duration of totality and annularity are near zero at the points where the changes between the two occur.[32]
Central eclipse
[edit]
Central eclipse is often used as a generic term for a total, annular, or hybrid eclipse.[33] This is, however, not completely correct: the definition of a central eclipse is an eclipse during which the central line of the umbra touches Earth's surface.
It is possible, though rare, that part of the umbra intersects with Earth (thus creating an annular or total eclipse), but not its central line. This is then called a non-central total or annular eclipse.[33] Gamma is a measure of how centrally the shadow strikes. The last (umbral yet) non-central solar eclipse was on April 29, 2014. This was an annular eclipse. The next non-central total solar eclipse will be on April 9, 2043.[34]
Eclipse phases
[edit]The visual phases observed during a total eclipse are called:[35]
- First contact—when the Moon's limb (edge) is exactly tangential to the Sun's limb.
- Second contact—starting with Baily's Beads (caused by light shining through valleys on the Moon's surface) and the diamond ring effect. Almost the entire disk is covered.
- Totality—the Moon obscures the entire disk of the Sun and only the solar corona is visible.
- Third contact—when the first bright light becomes visible and the Moon's shadow is moving away from the observer. Again a diamond ring may be observed.
- Fourth contact—when the trailing edge of the Moon ceases to overlap with the solar disk and the eclipse ends.
Occurrence and cycles
[edit]

A total solar eclipse is a rare event, recurring somewhere on Earth every 18 months on average,[37] yet is estimated to recur at any given location only every 360–410 years on average.[38] The total eclipse lasts for only a maximum of a few minutes at any location because the Moon's umbra moves eastward at over 1700 km/h (1100 mph; 470 m/s; 1500 ft/s).[39] Totality currently can never last more than 7 min 32 s. This value changes over the millennia and is currently decreasing. By the 8th millennium, the longest theoretically possible total eclipse will be less than 7 min 2 s.[20] The last time an eclipse longer than 7 minutes occurred was June 30, 1973 (7 min 3 sec). Observers aboard a Concorde supersonic aircraft were able to stretch totality for this eclipse to about 74 minutes by flying along the path of the Moon's umbra.[40] The next total eclipse exceeding seven minutes in duration will not occur until June 25, 2150. The longest total solar eclipse during the 11000 year period from 3000 BC to at least 8000 AD will occur on July 16, 2186, when totality will last 7 min 29 s.[20][41] For comparison, the longest total eclipse of the 20th century at 7 min 8 s occurred on June 20, 1955, and there will be no total solar eclipses over 7 min in duration in the 21st century.[42]
It is possible to predict other eclipses using eclipse cycles. The saros is probably the best known and one of the most accurate. A saros lasts 6585.3 days (a little over 18 years), which means that, after this period, a practically identical eclipse will occur. The most notable difference will be a westward shift of about 120° in longitude (due to the 0.3 days) and a little in latitude (north-south for odd-numbered cycles, the reverse for even-numbered ones). A saros series always starts with a partial eclipse near one of Earth's polar regions, then shifts over the globe through a series of annular or total eclipses, and ends with a partial eclipse at the opposite polar region. A saros series lasts 1226 to 1550 years and 69 to 87 eclipses, with about 40 to 60 of them being central.[43]
Frequency per year
[edit]Between two and five solar eclipses occur every year, with at least one per eclipse season. Since the Gregorian calendar was instituted in 1582, years that have had five solar eclipses were 1693, 1758, 1805, 1823, 1870, and 1935. The next occurrence will be 2206.[44] On average, there are about 240 solar eclipses each century.[45]
| January 5 | February 3 | June 30 | July 30 | December 25 |
|---|---|---|---|---|
| Partial (south) |
Partial (north) |
Partial (north) |
Partial (south) |
Annular (south) |
Saros 111 |
Saros 149 |
Saros 116 |
Saros 154 |
Saros 121 |
Final totality
[edit]Total solar eclipses are seen on Earth because of a fortuitous combination of circumstances. Even on Earth, the diversity of eclipses familiar to people today is a temporary (on a geological time scale) phenomenon. Hundreds of millions of years in the past, the Moon was closer to Earth and therefore apparently larger, so every solar eclipse was total or partial, and there were no annular eclipses. Due to tidal acceleration, the orbit of the Moon around Earth becomes approximately 3.8 cm more distant each year. Millions of years in the future, the Moon will be too far away to fully occlude the Sun, and no total eclipses will occur. In the same timeframe, the Sun may become brighter, making it appear larger in size.[46] Estimates of the time when the Moon will be unable to occlude the entire Sun when viewed from Earth range between 650 million[47] and 1.4 billion years in the future.[46]
Viewing
[edit]
Looking directly at the photosphere of the Sun (the bright disk of the Sun itself), even for just a few seconds, can cause permanent damage to the retina of the eye, because of the intense visible and invisible radiation that the photosphere emits. This damage can result in impairment of vision, up to and including blindness. The retina has no sensitivity to pain, and the effects of retinal damage may not appear for hours, so there is no warning that injury is occurring.[48][49]
Under normal conditions, the Sun is so bright that it is difficult to stare at it directly. However, during an eclipse, with so much of the Sun covered, it is easier and more tempting to stare at it. Looking at the Sun during an eclipse is as dangerous as looking at it outside an eclipse, except during the brief period of totality, when the Sun's disk is completely covered (totality occurs only during a total eclipse and only very briefly; it does not occur during a partial or annular eclipse). Viewing the Sun's disk through any kind of optical aid (binoculars, a telescope, or even an optical camera viewfinder) is extremely hazardous and can cause irreversible eye damage within a fraction of a second.[50][51]
Partial and annular eclipses
[edit]Viewing the Sun during partial and annular eclipses (and during total eclipses outside the brief period of totality) requires special eye protection, or indirect viewing methods if eye damage is to be avoided. The Sun's disk can be viewed using appropriate filtration to block the harmful part of the Sun's radiation. Sunglasses do not make viewing the Sun safe. Only properly designed and certified solar filters should be used for direct viewing of the Sun's disk.[52] Especially, self-made filters using common objects such as a floppy disk removed from its case, a Compact Disc, a black colour slide film, smoked glass, etc. must be avoided.[53][54]
The safest way to view the Sun's disk is by indirect projection.[55] This can be done by projecting an image of the disk onto a white piece of paper or card using a pair of binoculars (with one of the lenses covered), a telescope, or another piece of cardboard with a small hole in it (about 1 mm diameter), often called a pinhole camera. The projected image of the Sun can then be safely viewed; this technique can be used to observe sunspots, as well as eclipses. Care must be taken, however, to ensure that no one looks through the projector (telescope, pinhole, etc.) directly.[56] A kitchen colander with small holes can also be used to project multiple images of the partially eclipsed Sun onto the ground or a viewing screen. Viewing the Sun's disk on a video display screen (provided by a video camera or digital camera) is safe, although the camera itself may be damaged by direct exposure to the Sun. The optical viewfinders provided with some video and digital cameras are not safe. Securely mounting #14 welder's glass in front of the lens and viewfinder protects the equipment and makes viewing possible.[54] Professional workmanship is essential because of the dire consequences any gaps or detaching mountings will have. In the partial eclipse path, one will not be able to see the corona or nearly complete darkening of the sky. However, depending on how much of the Sun's disk is obscured, some darkening may be noticeable. If three-quarters or more of the Sun is obscured, then an effect can be observed by which the daylight appears to be dim, as if the sky were overcast, yet objects still cast sharp shadows.[57]
Totality
[edit]It is safe to observe the total phase of a solar eclipse directly only when the Sun's photosphere is completely covered by the Moon, and not before or after totality.[55] During this period, the Sun is too dim to be seen through filters. The Sun's faint corona will be visible, and the chromosphere, solar prominences, coronal streamers and possibly even a solar flare may be seen. At the end of totality, the same effects will occur in reverse order, and on the opposite side of the Moon.[58]
Eclipse chasing
[edit]A dedicated group of eclipse chasers have pursued the observation of solar eclipses when they occur around Earth.[59] A person who chases eclipses is known as an umbraphile, meaning shadow lover.[60] Umbraphiles travel for eclipses and use various tools to help view the sun including solar viewing glasses, also known as eclipse glasses, as well as telescopes.[61][62]
Photography
[edit]
The first known photograph of a solar eclipse was taken on July 28, 1851, by Julius Berkowski, using the daguerreotype process.[63][64]
Photographing an eclipse is possible with fairly common camera equipment. In order for the disk of the Sun/Moon to be easily visible, a fairly high magnification long focus lens is needed (at least 200 mm for a 35 mm camera), and for the disk to fill most of the frame, a longer lens is needed (over 500 mm). As with viewing the Sun directly, looking at it through the optical viewfinder of a camera can produce damage to the retina, so care is recommended.[65] Solar filters are required for digital photography even if an optical viewfinder is not used. Using a camera's live view feature or an electronic viewfinder is safe for the human eye, but the Sun's rays could potentially irreparably damage digital image sensors unless the lens is covered by a properly designed solar filter.[66]
Historical eclipses
[edit]
Historical eclipses are a very valuable resource for historians, in that they allow a few historical events to be dated precisely, from which other dates and ancient calendars may be deduced.[67] The oldest recorded solar eclipse was recorded on a clay tablet found at Ugarit, in modern Syria, with two plausible dates usually cited: 3 May 1375 BC or 5 March 1223 BC, the latter being favored by most recent authors on the topic.[68][69] A solar eclipse of June 15, 763 BC, mentioned in an Assyrian text is important for the chronology of the ancient Near East.[70] There have been other claims to date earlier eclipses. The legendary Chinese king Zhong Kang supposedly beheaded two astronomers, Hsi and Ho, who failed to predict an eclipse 4000 years ago.[71] Perhaps the earliest still-unproven claim is that of archaeologist Bruce Masse, who putatively links an eclipse that occurred on May 10, 2807, BC with a possible meteor impact in the Indian Ocean on the basis of several ancient flood myths that mention a total solar eclipse.[72]

Eclipses have been interpreted as omens, or portents.[73] The ancient Greek historian Herodotus wrote that Thales of Miletus predicted an eclipse that occurred during a battle between the Medes and the Lydians. Both sides put down their weapons and declared peace as a result of the eclipse.[74] The exact eclipse involved remains uncertain, although the issue has been studied by hundreds of ancient and modern authorities. One likely candidate took place on May 28, 585 BC, probably near the Halys river in Asia Minor.[75] An eclipse recorded by Herodotus before Xerxes departed for his expedition against Greece,[76] which is traditionally dated to 480 BC, was matched by John Russell Hind to an annular eclipse of the Sun at Sardis on February 17, 478 BC.[77] Alternatively, a partial eclipse was visible from Persia on October 2, 480 BC.[78] Herodotus also reports a solar eclipse at Sparta during the Second Persian invasion of Greece.[79] The date of the eclipse (August 1, 477 BC) does not match exactly the conventional dates for the invasion accepted by historians.[80]
In ancient China, where solar eclipses were known as an "eating of the Sun" (rìshí 日食), the earliest records of eclipses date to around 720 BC.[81] The 4th century BC astronomer Shi Shen described the prediction of eclipses by using the relative positions of the Moon and Sun.[82]
Attempts have been made to establish the exact date of Good Friday by assuming that the darkness described at Jesus's crucifixion was a solar eclipse. This research has not yielded conclusive results,[83][84] and Good Friday is recorded as being at Passover, which is held at the time of a full moon. Further, the darkness lasted from the sixth hour to the ninth, or three hours, which is much, much longer than the eight-minute upper limit for any solar eclipse's totality. Contemporary chronicles wrote about an eclipse at the beginning of May 664 that coincided with the beginning of the plague of 664 in the British isles.[85] In the Western hemisphere, there are few reliable records of eclipses before AD 800, until the advent of Arab and monastic observations in the early medieval period.[81]
A solar eclipse took place on January 27, 632 over Arabia during Muhammad's lifetime. Muhammad denied the eclipse had anything to do with his son dying earlier that day, saying "The sun and the moon do not eclipse because of the death of someone from the people but they are two signs amongst the signs of God."[86] The Cairo astronomer Ibn Yunus wrote that the calculation of eclipses was one of the many things that connect astronomy with the Islamic law, because it allowed knowing when a special prayer can be made.[87] The first recorded observation of the corona was made in Constantinople in AD 968.[78][81]

The first known telescopic observation of a total solar eclipse was made in France in 1706.[81] Nine years later, English astronomer Edmund Halley accurately predicted and observed the solar eclipse of May 3, 1715.[78][81] By the mid-19th century, scientific understanding of the Sun was improving through observations of the Sun's corona during solar eclipses. The corona was identified as part of the Sun's atmosphere in 1842, and the first photograph (or daguerreotype) of a total eclipse was taken of the solar eclipse of July 28, 1851.[78] Spectroscope observations were made of the solar eclipse of August 18, 1868, which helped to determine the chemical composition of the Sun.[78]
John Fiske summed up myths about the solar eclipse like this in his 1872 book Myth and Myth-Makers,
the myth of Hercules and Cacus, the fundamental idea is the victory of the solar god over the robber who steals the light. Now whether the robber carries off the light in the evening when Indra has gone to sleep, or boldly rears his black form against the sky during the daytime, causing darkness to spread over the earth, would make little difference to the framers of the myth. To a chicken a solar eclipse is the same thing as nightfall, and he goes to roost accordingly. Why, then, should the primitive thinker have made a distinction between the darkening of the sky caused by black clouds and that caused by the rotation of the earth? He had no more conception of the scientific explanation of these phenomena than the chicken has of the scientific explanation of an eclipse. For him it was enough to know that the solar radiance was stolen, in the one case as in the other, and to suspect that the same demon was to blame for both robberies.[88]
Particular observations, phenomena and impact
[edit]
A total solar eclipse provides a rare opportunity to observe the corona (the outer layer of the Sun's atmosphere). Normally this is not visible because the photosphere is much brighter than the corona. According to the point reached in the solar cycle, the corona may appear small and symmetric, or large and fuzzy. It is very hard to predict this in advance.[89]
Phenomena associated with eclipses include shadow bands (also known as flying shadows), which are similar to shadows on the bottom of a swimming pool. They occur only just prior to and after totality, when a narrow solar crescent acts as an anisotropic light source.[90] As the light filters through leaves of trees during a partial eclipse, the overlapping leaves create natural pinholes, displaying mini eclipses on the ground.[91]
1919 observations
[edit]
The observation of a total solar eclipse of May 29, 1919, helped to confirm Einstein's theory of general relativity. By comparing the apparent distance between stars in the constellation Taurus, with and without the Sun between them, Arthur Eddington stated that the theoretical predictions about gravitational lenses were confirmed.[92] The observation with the Sun between the stars was possible only during totality since the stars are then visible. Though Eddington's observations were near the experimental limits of accuracy at the time, work in the later half of the 20th century confirmed his results.[93][94]
Gravity anomalies
[edit]There is a long history of observations of gravity-related phenomena during solar eclipses, especially during the period of totality. Maurice Allais reported observing unusual and unexplained movements during solar eclipses in both 1954 and 1959.[95] The reality of this phenomenon, named the Allais effect, has remained controversial. Similarly, in 1970, Saxl and Allen observed the sudden change in motion of a torsion pendulum; this phenomenon is called the Saxl effect.[96]
Observation during the 1997 solar eclipse by Wang et al. suggested a possible gravitational shielding effect,[97] which generated debate. In 2002, Wang and a collaborator published detailed data analysis, which suggested that the phenomenon still remains unexplained.[98]
Eclipses and transits
[edit]In principle, the simultaneous occurrence of a solar eclipse and a transit of a planet is possible. But these events are extremely rare because of their short durations. The next anticipated simultaneous occurrence of a solar eclipse and a transit of Mercury will be on July 5, 6757, and a solar eclipse and a transit of Venus is expected on April 5, 15232.[99]
More common, but still infrequent, is a conjunction of a planet (especially, but not only, Mercury or Venus) at the time of a total solar eclipse, in which event the planet will be visible very near the eclipsed Sun, when without the eclipse it would have been lost in the Sun's glare. At one time, some scientists hypothesized that there may be a planet (often given the name Vulcan) even closer to the Sun than Mercury; the only way to confirm its existence would have been to observe it in transit or during a total solar eclipse. No such planet was ever found, and general relativity has since explained the observations that led astronomers to suggest that Vulcan might exist.[100]
Artificial satellites
[edit]
Artificial satellites can also pass in front of the Sun as seen from Earth, but none is large enough to cause an eclipse. At the altitude of the International Space Station, for example, an object would need to be about 3.35 km (2.08 mi) across to blot the Sun out entirely. These transits are difficult to watch because the zone of visibility is very small. The satellite passes over the face of the Sun in about a second, typically. As with a transit of a planet, it will not get dark.[101]
Observations of eclipses from spacecraft or artificial satellites orbiting above Earth's atmosphere are not subject to weather conditions. The crew of Gemini 12 observed a total solar eclipse from space in 1966.[102] The partial phase of the 1999 total eclipse was visible from Mir.[103]
As of 2025, a pair of satellites launched by the European Space Agency (Proba-3 mission) began creating on-demand eclipses relative to one another.[104] These eclipses cannot be seen from earth, but are captured by imaging from one satellite while the other interposes itself between the sun and the imaging satellite.[104]
Impact
[edit]The solar eclipse of March 20, 2015, was the first occurrence of an eclipse estimated to potentially have a significant impact on the power system, with the electricity sector taking measures to mitigate any impact. The continental Europe and Great Britain synchronous areas were estimated to have about 90 gigawatts of solar power and it was estimated that production would temporarily decrease by up to 34 GW compared to a clear sky day.[105][106]
Eclipses may cause the temperature to decrease by 3 °C (5 °F), with wind power potentially decreasing as winds are reduced by 0.7 meters (2.3 ft) per second.[107]
In addition to the drop in light level and air temperature, animals change their behavior during totality. For example, birds and squirrels return to their nests and crickets chirp.[108]
Recent and forthcoming solar eclipses
[edit]
Eclipses occur only in the eclipse season, when the Sun is close to either the ascending or descending node of the Moon. Each eclipse is separated by one, five or six lunations (synodic months), and the midpoint of each season is separated by 173.3 days, which is the mean time for the Sun to travel from one node to the next. The period is a little less than half a calendar year because the lunar nodes slowly regress. Because 223 synodic months is roughly equal to 239 anomalistic months and 242 draconic months, eclipses with similar geometry recur 223 synodic months (about 6,585.3 days) apart. This period (18 years 11.3 days) is a saros. Because 223 synodic months is not identical to 239 anomalistic months or 242 draconic months, saros cycles do not endlessly repeat. Each cycle begins with the Moon's shadow crossing Earth near the north or south pole, and subsequent events progress toward the other pole until the Moon's shadow misses Earth and the series ends.[14] Saros cycles are numbered; currently, cycles 117 to 156 are active.[109]
2018–2021
[edit]| Solar eclipse series sets from 2018 to 2021 | ||||||
|---|---|---|---|---|---|---|
| Ascending node | Descending node | |||||
| Saros | Map | Gamma | Saros | Map | Gamma | |
| 117 Partial in Melbourne, Australia |
July 13, 2018 Partial |
−1.35423 | 122 Partial in Nakhodka, Russia |
January 6, 2019 Partial |
1.14174 | |
| 127 Totality in La Serena, Chile |
July 2, 2019 Total |
−0.64656 | 132 Annularity in Jaffna, Sri Lanka |
December 26, 2019 Annular |
0.41351 | |
| 137 Annularity in Beigang, Yunlin, Taiwan |
June 21, 2020 Annular |
0.12090 | 142 Totality in Gorbea, Chile |
December 14, 2020 Total |
−0.29394 | |
| 147 Partial in Halifax, Canada |
June 10, 2021 Annular |
0.91516 | 152 From HMS Protector off South Georgia |
December 4, 2021 Total |
−0.95261 | |
2022–2025
[edit]| Solar eclipse series sets from 2022 to 2025 | ||||||
|---|---|---|---|---|---|---|
| Ascending node | Descending node | |||||
| Saros | Map | Gamma | Saros | Map | Gamma | |
| 119 Partial in CTIO, Chile |
April 30, 2022 Partial |
−1.19008 | 124 Partial from Saratov, Russia |
October 25, 2022 Partial |
1.07014 | |
| 129 Partial in Magetan, Indonesia |
April 20, 2023 Hybrid |
−0.39515 | 134 Annularity in Hobbs, NM, USA |
October 14, 2023 Annular |
0.37534 | |
| 139 Totality in Dallas, TX, USA |
April 8, 2024 Total |
0.34314 | 144 Annularity in Santa Cruz Province, Argentina |
October 2, 2024 Annular |
−0.35087 | |
| 149 | March 29, 2025 Partial |
1.04053 | 154 | September 21, 2025 Partial |
−1.06509 | |
2026–2029
[edit]| Solar eclipse series sets from 2026 to 2029 | ||||||
|---|---|---|---|---|---|---|
| Ascending node | Descending node | |||||
| Saros | Map | Gamma | Saros | Map | Gamma | |
| 121 | February 17, 2026 Annular |
−0.97427 | 126 | August 12, 2026 Total |
0.89774 | |
| 131 | February 6, 2027 Annular |
−0.29515 | 136 | August 2, 2027 Total |
0.14209 | |
| 141 | January 26, 2028 Annular |
0.39014 | 146 | July 22, 2028 Total |
−0.60557 | |
| 151 | January 14, 2029 Partial |
1.05532 | 156 | July 11, 2029 Partial |
−1.41908 | |
See also
[edit]- Lists of solar eclipses
- List of films featuring eclipses
- Apollo–Soyuz: First joint U.S.–Soviet space flight. Mission included an arranged eclipse of the Sun by the Apollo module to allow instruments on the Soyuz to take photographs of the solar corona.
- Eclipse chasing: Travel to eclipse locations for study and enjoyment
- Occultation: Generic term for occlusion of an object by another object that passes between it and the observer, thus revealing (for example) the presence of an exoplanet orbiting a distant star by eclipsing it as seen from Earth
- Eclipses in history and culture: treatment of solar and lunar eclipses by historical and contemporary society and religion
- Solar eclipses in fiction
- Solar eclipses on the Moon: Eclipse of the Sun by planet Earth, as seen from the Moon
- Lunar eclipse: Solar eclipse of the Moon, as seen from Earth; the shadow cast on the Moon by that eclipse
- Transit of Venus: Passage of the planet Venus between the Sun and Earth, as seen from Earth. Technically a partial eclipse.
- Transit of Deimos from Mars: Passage of the Martian moon Deimos between the Sun and Mars, as seen from Mars
- Transit of Phobos from Mars: Passage of the Martian moon Phobos between the Sun and Mars, as seen from Mars
Footnotes
[edit]References
[edit]- ^ "What is an eclipse?". European Space Agency. Archived from the original on 2018-08-04. Retrieved 2018-08-04.
- ^ a b Littmann, Mark; Espenak, Fred; Willcox, Ken (2008). Totality: Eclipses of the Sun. Oxford University Press. pp. 18–19. ISBN 978-0-19-953209-4.
- ^ Five solar eclipses occurred in 1935.NASA (September 6, 2009). "Five Millennium Catalog of Solar Eclipses". NASA Eclipse Web Site. Fred Espenak, Project and Website Manager. Archived from the original on April 29, 2010. Retrieved January 26, 2010.
- ^ Koukkos, Christina (May 14, 2009). "Eclipse Chasing, in Pursuit of Total Awe". The New York Times. Archived from the original on June 26, 2018. Retrieved January 15, 2012.
- ^ Pasachoff, Jay M. (July 10, 2010). "Why I Never Miss a Solar Eclipse". The New York Times. Archived from the original on June 26, 2018. Retrieved January 15, 2012.
- ^ Mobberley, pp. 30–38
- ^ a b c Harrington, pp. 4–5
- ^ Hipschman, Ron. "Why Eclipses Happen". Exploratorium. Archived from the original on December 27, 2015. Retrieved January 14, 2012.
- ^ Brewer, Bryan (January 14, 1998). "What Causes an Eclipse?". Earth View. Archived from the original on January 2, 2013. Retrieved January 14, 2012.
- ^ NASA – Eclipse 99 – Frequently Asked Questions Archived 2010-05-27 at the Wayback Machine – There is a mistake in the How long will we continue to be able to see total eclipses of the Sun? answer, "...the Sun's angular diameter varies from 32.7 minutes of arc when the Earth is at its farthest point in its orbit (aphelion), and 31.6 arc minutes when it is at its closest (perihelion)." It should appear smaller when farther, so the values should be swapped.
- ^ Steel, pp. 319–321
- ^ Steel, pp. 317–319
- ^ Harrington, pp. 5–7
- ^ a b Espenak, Fred (August 28, 2009). "Periodicity of Solar Eclipses". NASA Eclipse web site. Greenbelt, MD: NASA Goddard Space Flight Center. Archived from the original on November 12, 2020. Retrieved January 15, 2012.
- ^ Espenak, Fred; Meeus, Jean (January 26, 2007). "Five Millennium Catalog of Solar Eclipses: -1999 to +3000". NASA Eclipse web site. Greenbelt, MD: NASA Goddard Space Flight Center. Archived from the original on October 24, 2020. Retrieved January 15, 2012.
- ^ Mobberley, pp. 33–37
- ^ "How do eclipses such as the one on Wednesday 14 November 2012 occur?". Sydney Observatory. Archived from the original on 29 April 2013. Retrieved 20 March 2015.
- ^ Steel, pp. 52–53
- ^ a b Seidelmann, P. Kenneth; Urban, Sean E., eds. (2013). Explanatory Supplement to the Astronomical Almanac (3rd ed.). University Science Books. ISBN 978-1-891389-85-6.
- ^ a b c d Meeus, J. (December 2003). "The maximum possible duration of a total solar eclipse". Journal of the British Astronomical Association. 113 (6): 343–348. Bibcode:2003JBAA..113..343M.
- ^ M. Littman, et al.
- ^ a b c d e f Harrington, pp. 9–11
- ^ "Solar Eclipses". University of Tennessee. Archived from the original on June 9, 2015. Retrieved January 15, 2012.
- ^ "How Is the Sun Completely Blocked in an Eclipse?". NASA Space Place. NASA. 2009. Archived from the original on 2021-01-19. Retrieved 2019-09-01.
- ^ Steel, p. 351
- ^ Baylor University Department of Physics (2024). "What is a solar eclipse?". Baylor University. Retrieved April 12, 2024.
There are three main types of solar eclipses: Total solar eclipse, Partial solar eclipse, Annular solar eclipse
- ^ a b c "What Are the Three Types of Solar Eclipses?". Exploratorium. 17 April 2023. Retrieved 11 Oct 2023.
- ^ Harrington, pp. 7–8
- ^ "Eclipse: Who? What? Where? When? and How? | Total Solar Eclipse 2017". eclipse2017.nasa.gov. Archived from the original on 2017-09-18. Retrieved 2017-09-21.
- ^ a b Villalpando, Roberto (September 15, 2023). "October eclipse will be annular, not annual, but oversized glasses show how confusing it can be". San Antonio Express-News. Retrieved April 11, 2024.
Annular means of, relating to or forming a ring [...] it has its roots in the Latin word for ring, 'anulus'. [...] Annual, on the other hand, means occurring every year or once a year. The word also has a Latin ancestor: 'annus', which means year.
- ^ "Transit of Venus, Sun–Earth Day 2012". nasa.gov. Archived from the original on January 14, 2016. Retrieved February 7, 2016.
- ^ Espenak, Fred (September 26, 2009). "Solar Eclipses for Beginners". MrEclipse.com. Archived from the original on May 24, 2015. Retrieved January 15, 2012.
- ^ a b Espenak, Fred (January 6, 2009). "Central Solar Eclipses: 1991–2050". NASA Eclipse web site. Greenbelt, MD: NASA Goddard Space Flight Center. Archived from the original on January 8, 2021. Retrieved January 15, 2012.
- ^ Verbelen, Felix (November 2003). "Solar Eclipses on Earth, 1001 BC to AD 2500". online.be. Archived from the original on August 3, 2019. Retrieved January 15, 2012.
- ^ Harrington, pp. 13–14; Steel, pp. 266–279
- ^ Espenak, Fred (March 24, 2008). "World Atlas of Solar Eclipse Paths". NASA Eclipse web site. NASA Goddard Space Flight Center. Archived from the original on July 14, 2012. Retrieved January 15, 2012.
- ^ Steel, p. 4
- ^ For 360 years, see Harrington, p. 9; for 410 years, see Steel, p. 31
- ^ Mobberley, pp. 33–36; Steel, p. 258
- ^ Beckman, J.; Begot, J.; Charvin, P.; Hall, D.; Lena, P.; Soufflot, A.; Liebenberg, D.; Wraight, P. (1973). "Eclipse Flight of Concorde 001". Nature. 246 (5428): 72–74. Bibcode:1973Natur.246...72B. doi:10.1038/246072a0. S2CID 10644966.
- ^ Stephenson, F. Richard (1997). Historical Eclipses and Earth's Rotation. Cambridge University Press. p. 54. doi:10.1017/CBO9780511525186. ISBN 0-521-46194-4. Archived from the original on 2020-08-01. Retrieved 2012-01-04.
- ^ Mobberley, p. 10
- ^ Espenak, Fred (August 28, 2009). "Eclipses and the Saros". NASA Eclipse web site. NASA Goddard Space Flight Center. Archived from the original on May 24, 2012. Retrieved January 15, 2012.
- ^ Pogo, Alexander (1935). "Calendar years with five solar eclipses". Popular Astronomy. Vol. 43. p. 412. Bibcode:1935PA.....43..412P.
- ^ "What are solar eclipses and how often do they occur?". timeanddate.com. Archived from the original on 2017-02-02. Retrieved 2014-11-23.
- ^ a b Walker, John (July 10, 2004). "Moon near Perigee, Earth near Aphelion". Fourmilab. Archived from the original on December 8, 2013. Retrieved March 7, 2010.
- ^ Mayo, Lou. "WHAT'S UP? The Very Last Solar Eclipse!". NASA. Archived from the original on 2017-08-22. Retrieved 22 August 2017.
- ^ Espenak, Fred (July 11, 2005). "Eye Safety During Solar Eclipses". NASA Eclipse web site. NASA Goddard Space Flight Center. Archived from the original on July 16, 2012. Retrieved January 15, 2012.
- ^ Dobson, Roger (August 21, 1999). "UK hospitals assess eye damage after solar eclipse". British Medical Journal. 319 (7208): 469. doi:10.1136/bmj.319.7208.469. PMC 1116382. PMID 10454393.
- ^ MacRobert, Alan M. (8 August 2006). "How to Watch a Partial Solar Eclipse Safely". Sky & Telescope. Retrieved August 4, 2007.
- ^ Chou, B. Ralph (July 11, 2005). "Eye safety during solar eclipses". NASA Eclipse web site. NASA Goddard Space Flight Center. Archived from the original on November 14, 2020. Retrieved January 15, 2012.
- ^ Littmann, Mark; Willcox, Ken; Espenak, Fred (1999). "Observing Solar Eclipses Safely". MrEclipse.com. Archived from the original on July 26, 2020. Retrieved January 15, 2012.
- ^ Chou, B. Ralph (January 20, 2008). "Eclipse Filters". MrEclipse.com. Archived from the original on November 27, 2020. Retrieved January 4, 2012.
- ^ a b "Solar Viewing Safety". Perkins Observatory. Archived from the original on July 14, 2020. Retrieved January 15, 2012.
- ^ a b Harrington, p. 25
- ^ Harrington, p. 26
- ^ Harrington, p. 40
- ^ Littmann, Mark; Willcox, Ken; Espenak, Fred (1999). "The Experience of Totality". MrEclipse.com. Archived from the original on February 4, 2012. Retrieved January 15, 2012.
- ^ Kate Russo (2012). Total Addiction: The Life of an Eclipse Chaser. Springer Science & Business Media. ISBN 978-3-642-30481-1. Archived from the original on 9 December 2019. Retrieved 24 August 2017.
- ^ Kelly, Pat (2017-07-06). "Umbraphile, Umbraphilia, Umbraphiles, and Umbraphiliacs – Solar Eclipse with the Sol Alliance". Solar Eclipse with the Sol Alliance. Archived from the original on 2019-08-13. Retrieved 2017-08-24.
- ^ "How to View the 2017 Solar Eclipse Safely". eclipse2017.nasa.gov. Archived from the original on 2017-08-24. Retrieved 2017-08-24.
- ^ Wright, Andy (2017-08-16). "Chasing Totality: A Look Into the World of Umbraphiles". Atlas Obscura. Archived from the original on 2020-12-14. Retrieved 2017-08-24.
- ^ Weitering, Hanneke (2017-07-28). "1st Photo of a Total Solar Eclipse Was Taken 166 Years Ago Today". Space.com. Retrieved 2024-04-08.
- ^ Farber, Madeline (2017-08-11). "This Is the First-Ever Photo of a Total Solar Eclipse". TIME. Retrieved 2024-04-09.
- ^ Kramer, Bill. "Photographing a Total Solar Eclipse". Eclipse-chasers.com. Archived from the original on January 29, 2009. Retrieved March 7, 2010.
- ^ Vorenkamp, Todd (April 2017). "How to Photograph a Solar Eclipse". B&H Photo Video. Archived from the original on July 1, 2019. Retrieved August 19, 2017.
- ^ Acta Eruditorum. Leipzig. 1762. p. 168. Archived from the original on 2020-07-31. Retrieved 2018-06-06.
- ^ "Solar Physics Historical Timeline (1223 BC – 200 BC) | High Altitude Observatory". www2.hao.ucar.edu. Retrieved 2023-12-14.
- ^ Smith, Kiona N. "People Recorded A Total Solar Eclipse For The First Time 3,241 Years Ago". Forbes. Retrieved 2023-12-14.
- ^ van Gent, Robert Harry. "Astronomical Chronology". University of Utrecht. Archived from the original on July 28, 2020. Retrieved January 15, 2012.
- ^ Harrington, p. 2
- ^ Blakeslee, Sandra (November 14, 2006). "Ancient Crash, Epic Wave". The New York Times. Archived from the original on April 11, 2009. Retrieved November 14, 2006.
- ^ Steel, p. 1
- ^ Steel, pp. 84–85
- ^ Le Conte, David (December 6, 1998). "Eclipse Quotations". MrEclipse.com. Archived from the original on October 17, 2020. Retrieved January 8, 2011.
- ^ Herodotus. Book VII. p. 37. Archived from the original on 2008-08-19. Retrieved 2008-07-13.
- ^ Chambers, G. F. (1889). A Handbook of Descriptive and Practical Astronomy. Oxford: Clarendon Press. p. 323.
- ^ a b c d e Espenak, Fred. "Solar Eclipses of Historical Interest". NASA Eclipse web site. NASA Goddard Space Flight Center. Archived from the original on March 9, 2008. Retrieved December 28, 2011.
- ^ Herodotus. Book IX. p. 10. Archived from the original on 2020-07-26. Retrieved 2008-07-14.
- ^ Schaefer, Bradley E. (May 1994). "Solar Eclipses That Changed the World". Sky & Telescope. Vol. 87, no. 5. pp. 36–39. Bibcode:1994S&T....87...36S.
- ^ a b c d e Stephenson, F. Richard (1982). "Historical Eclipses". Scientific American. Vol. 247, no. 4. pp. 154–163. Bibcode:1982SciAm.247d.154S.
- ^ Needham, Joseph (1986). Science and Civilization in China: Volume 3. Taipei: Caves Books. pp. 411–413. OCLC 48999277.
- ^ Humphreys, C. J.; Waddington, W. G. (1983). "Dating the Crucifixion". Nature. 306 (5945): 743–746. Bibcode:1983Natur.306..743H. doi:10.1038/306743a0. S2CID 4360560.
- ^ Kidger, Mark (1999). The Star of Bethlehem: An Astronomer's View. Princeton, NJ: Princeton University Press. pp. 68–72. ISBN 978-0-691-05823-8.
- ^ Ó Cróinín, Dáibhí (13 May 2020). "Reeling in the years: why 664 AD was a terrible year in Ireland". rte.ie. Archived from the original on 2021-01-08. Retrieved January 9, 2021.
- ^ "Translation of Sahih Bukhari, Book 18".
- ^ Regis Morelon (1996). "General survey of Arabic astronomy". In Roshdi Rashed (ed.). Encyclopedia of the History of Arabic Science. Vol. I. Routledge. p. 15.
- ^ Fiske, John (1997). Myths and Myth-Makers Old Tales and Superstitions Interpreted by Comparative Mythology. Archived from the original on July 26, 2020. Retrieved February 12, 2017 – via Project Gutenberg.
- ^ "The science of eclipses". ESA. September 28, 2004. Archived from the original on August 1, 2012. Retrieved August 4, 2007.
- ^ Dravins, Dainis. "Flying Shadows". Lund Observatory. Archived from the original on July 26, 2020. Retrieved January 15, 2012.
- ^ Johnson-Groh, Mara (10 August 2017). "Five Tips from NASA for Photographing the Total Solar Eclipse on Aug. 21". NASA. Archived from the original on 18 August 2020. Retrieved 21 September 2017.
- ^ Dyson, F.W.; Eddington, A.S.; Davidson, C.R. (1920). "A Determination of the Deflection of Light by the Sun's Gravitational Field, from Observations Made at the Solar eclipse of May 29, 1919". Phil. Trans. Roy. Soc. A. 220 (571–81): 291–333. Bibcode:1920RSPTA.220..291D. doi:10.1098/rsta.1920.0009. Archived from the original on November 3, 2020. Retrieved August 27, 2019.
- ^ "Relativity and the 1919 eclipse". ESA. September 13, 2004. Archived from the original on October 21, 2012. Retrieved January 11, 2011.
- ^ Steel, pp. 114–120
- ^ Allais, Maurice (1959). "Should the Laws of Gravitation be Reconsidered?". Aero/Space Engineering. 9: 46–55.
- ^ Saxl, Erwin J.; Allen, Mildred (1971). "1970 solar eclipse as 'seen' by a torsion pendulum". Physical Review D. 3 (4): 823–825. Bibcode:1971PhRvD...3..823S. doi:10.1103/PhysRevD.3.823.
- ^ Wang, Qian-shen; Yang, Xin-she; Wu, Chuan-zhen; Guo, Hong-gang; Liu, Hong-chen; Hua, Chang-chai (2000). "Precise measurement of gravity variations during a total solar eclipse". Physical Review D. 62 (4): 041101(R). arXiv:1003.4947. Bibcode:2000PhRvD..62d1101W. doi:10.1103/PhysRevD.62.041101. S2CID 6846335.
- ^ Yang, X. S.; Wang, Q. S. (2002). "Gravity anomaly during the Mohe total solar eclipse and new constraint on gravitational shielding parameter". Astrophysics and Space Science. 282 (1): 245–253. Bibcode:2002Ap&SS.282..245Y. doi:10.1023/A:1021119023985. S2CID 118497439.
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- ^ a b Prillaman, McKenzie (September 2025). "Spacecraft produce eclipse on demand". News: Astronomy. Science News. Vol. 207, no. 9. p. 13.
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Bibliography
[edit]- Mucke, Hermann; Meeus, Jean (1992). Canon of Solar Eclipses −2003 to +2526 (2 ed.). Vienna: Astronomisches Büro.
- Harrington, Philip S. (1997). Eclipse! The What, Where, When, Why and How Guide to Watching Solar and Lunar Eclipses. New York: John Wiley and Sons. ISBN 0-471-12795-7.
- Steel, Duncan (1999). Eclipse: The celestial phenomenon which has changed the course of history. London: Headline. ISBN 0-7472-7385-5.
- Mobberley, Martin (2007). Total Solar Eclipses and How to Observe Them. Astronomers' Observing Guides. New York: Springer. ISBN 978-0-387-69827-4.
- Espenak, Fred (2015). Thousand Year Canon of Solar Eclipses 1501 to 2500. Portal AZ: Astropixels Publishing. ISBN 978-1-941983-02-7.
- Espenak, Fred (2016). 21st Century Canon of Solar Eclipses. Portal AZ: Astropixels Publishing. ISBN 978-1-941983-12-6.
- Fotheringham, John Knight (1921). Historical eclipses: being the Halley lecture delivered 17 May 1921. Oxford: Clarendon Press.
External links
[edit]- NASA Eclipse Web Site, with information on future eclipses and eye safety information
- NASA Eclipse Web Site (older version)
- Eclipsewise, Fred Espenak's new eclipse site
- Andrew Lowe's Eclipse Page, with maps and circumstances for 5000 years of solar eclipses
- A Guide to Eclipse Activities for Educators, Explaining eclipses in educational settings
- Detailed eclipse explanations and predictions, Hermit Eclipse
- Eclipse Photography, Prof. Miroslav Druckmüller
- Animated maps of August 21, 2017 solar eclipses, Larry Koehn
- Five Millennium (−1999 to +3000) Canon of Solar Eclipses Database, Xavier M. Jubier
- Animated explanation of the mechanics of a solar eclipse Archived 2013-05-25 at the Wayback Machine, University of South Wales
- Eclipse Image Gallery Archived 2016-10-15 at the Wayback Machine, The World at Night
- Ring of Fire Eclipse: 2012, Photos
- . Collier's New Encyclopedia. 1921.
- Centered and aligned video recording of Total Solar Eclipse 20th March 2015 on YouTube
- Solar eclipse photographs taken from the Lick Observatory from the Lick Observatory Records Digital Archive, UC Santa Cruz Library’s Digital Collections Archived 2020-06-05 at the Wayback Machine
- Video with Total Solar Eclipse March 09 2016 (from the beginning to the total phase) on YouTube
- Total Solar Eclipse Shadow on Earth March 09 2016 CIMSSSatelite
- List of all solar eclipses
- National Geographic Solar Eclipse 101 video Archived 2018-08-04 at the Wayback Machine
Wikiversity has a solar eclipse lab that students can do on any sunny day.
Solar eclipse
View on GrokipediaFundamentals
Definition
A solar eclipse occurs when the Moon passes between Earth and the Sun, thereby blocking some or all of the Sun's light from reaching Earth and casting a shadow on the planet's surface.[2] This alignment temporarily obscures the Sun as viewed from specific locations on Earth, creating a dramatic celestial event driven by the relative positions of these three bodies in the solar system.[1] Solar eclipses can only happen during the new moon phase, when the Moon is positioned between Earth and the Sun along the ecliptic plane, aligning the three bodies nearly in a straight line.[8] The Moon's shadow on Earth consists of two primary regions: the umbra, a central cone of total darkness where the Sun is completely obscured, and the surrounding penumbra, an area of partial shading where the Sun appears partially covered.[2] In cases where the Moon is too distant to fully cover the Sun, an additional region called the antumbra forms beyond the umbra tip, allowing a ring of sunlight to remain visible.[9] During a solar eclipse, the affected region on Earth experiences a noticeable darkening of the daytime sky, resembling twilight or dawn, depending on the eclipse's extent, while unaffected areas see no change.[10] This phenomenon is visible only from the narrow path swept by the Moon's shadow across Earth's surface, limiting observation to specific geographic areas.[1] Globally, solar eclipses occur between two and five times per year on average, though the exact number varies due to the orbital inclinations of Earth and the Moon.Types
Solar eclipses are classified into four primary types based on the Moon's apparent size relative to the Sun and the nature of its shadow cast on Earth: total, annular, partial, and hybrid. These categories arise from variations in the Moon's distance from Earth during the alignment with the Sun, which affects whether the Moon's disk fully obscures the Sun or leaves a portion visible. The shadow consists of the umbra (the darkest central region), the antumbra (the extension beyond the umbra's tip), and the penumbra (the outer partial shadow).[1] A total solar eclipse occurs when the Moon is close enough to Earth that its umbra fully reaches the surface, completely blocking the Sun's disk along a narrow path of totality. In this path, typically 100-200 kilometers wide, the sky darkens to twilight levels, stars become visible, and the Sun's corona is revealed as a glowing halo. Outside this path but within the penumbra, the eclipse appears partial. Total eclipses happen when the Moon is near its perigee, making it appear larger than the Sun.[1] An annular solar eclipse takes place when the Moon is farther from Earth, near apogee, causing it to appear smaller than the Sun; the umbra does not reach Earth, but the antumbra does, resulting in a bright ring of sunlight—known as the "ring of fire"—surrounding the Moon's silhouette. The path of annularity is similar in width to that of totality in total eclipses, with partial phases visible over a broader region. This type emphasizes the Sun's greater actual size compared to the Moon, despite their similar angular diameters from Earth.[1] A partial solar eclipse is observed when only the Moon's penumbra touches Earth, obscuring a portion of the Sun without the umbra or antumbra intersecting the surface. The Sun appears as a crescent, with the extent of coverage varying by location—the deepest obscuration near the edges of central eclipse paths and less elsewhere. Partial eclipses are visible over large areas, often spanning continents, and accompany every total or annular event.[1] Hybrid solar eclipses, also called annular-total eclipses, occur when the Moon's shadow transitions between umbra and antumbra along its path due to Earth's curvature; observers in some sections experience totality, while others see annularity. This rare configuration requires precise alignment where the shadow cone's tip just grazes Earth's varying topography. The path remains narrow, with partial visibility surrounding it.[1] Solar eclipses are further distinguished as central or non-central. Central eclipses—encompassing total, annular, and hybrid types—occur when the axis of the Moon's shadow cone intersects Earth's surface, producing a defined path where the umbra or antumbra falls. Non-central eclipses are partial only, as the shadow axis misses Earth entirely, with only the penumbra affecting observers. Non-central total or annular events are possible but classified separately when the cone merely grazes the surface without full intersection.[9] Total solar eclipses occur globally about every 18 months on average, though their paths cover only a small fraction of Earth's surface each time. For any specific location, the average interval between total eclipses is approximately 366 years, highlighting their local rarity.[11][4]Terminology and Geometry
Key terms
In solar eclipses, the progression of events is marked by four key contacts, which define the phases of the eclipse. First contact occurs at the instant when the Moon's disk first touches the Sun's disk, marking the beginning of the partial phase as the Moon starts to obscure the Sun.[9] Second contact marks the start of the central phase: in total eclipses, when the Moon's disk fully covers the Sun; in annular eclipses, when the Moon's disk is entirely within the Sun's disk, initiating the total or annular phase of the eclipse.[9] Third contact marks the end of the central phase: in total eclipses, when the Moon begins to uncover the Sun; in annular eclipses, when the Moon begins to exit the Sun's disk, resuming partial obscuration.[9] Fourth contact concludes the partial phase when the Moon's disk fully separates from the Sun's disk.[9] During the transitions at second and third contact in a total eclipse, distinctive optical effects become visible due to the Moon's irregular edge. Baily's beads appear as a series of bright spots of sunlight shining through the valleys on the Moon's limb just before and after totality.[12] Immediately following or preceding this, the diamond ring effect manifests as a single brilliant point of sunlight—resembling a diamond—against the dim solar corona, creating a striking ring-like appearance around the Moon.[10] A central eclipse refers to any solar eclipse where the central axis of the Moon's shadow cone intersects Earth's surface, encompassing total, annular, and hybrid varieties along the path of centrality.[9] The axis of centrality, also known as the shadow axis, traces the centerline of this shadow cone as it moves across Earth.[13] The parameter gamma quantifies the misalignment of this axis from Earth's center, measured in Earth equatorial radii, with values near zero indicating a more central passage.[9] During totality in a total eclipse, features of the Sun's atmosphere become observable. Solar prominences are dense clouds of plasma suspended above the Sun's surface by magnetic fields, appearing as bright pink arcs or loops at the limb.[10] The corona, the Sun's outermost atmosphere, is a faint, pearly-white halo of ionized gas extending millions of kilometers, fully revealed only when the Moon completely blocks the Sun's disk.[9]Geometric principles
A solar eclipse occurs due to the specific geometric alignment of the Earth, Moon, and Sun within the solar system. The Moon's orbit around Earth is inclined by approximately 5.145° relative to the ecliptic plane, which is the plane of Earth's orbit around the Sun. This tilt means that the Moon's path crosses the ecliptic at two points known as the ascending node (where the Moon moves northward) and the descending node (where it moves southward). Eclipses can only happen when the Moon is positioned near one of these nodes during its orbital motion, as this alignment allows the Moon to pass directly between Earth and the Sun or for Earth to pass between the Moon and the Sun. The fundamental geometric condition for a solar eclipse is syzygy, the near-perfect straight-line alignment of the Sun, Moon, and Earth, with the Moon interposed between the other two bodies. Without this collinear configuration, the Moon's shadow would not project onto Earth's surface in a way that obscures the Sun from observers on the planet. The rarity of such precise alignments, combined with the orbital inclination, limits solar eclipses to occurring only about twice per year on average, and visible from any given location much less frequently. The geometry of the eclipse involves the projection of the Moon's shadow onto Earth, consisting of two main regions: the umbra and the penumbra. The umbra is the dark, central cone where the Sun is completely obscured by the Moon, extending from the Moon's surface for about 373,000 km toward Earth—reaching the planet's surface only when the Moon is sufficiently close in its elliptical orbit. Beyond the umbra tip lies the antumbra, where the Moon appears smaller than the Sun, resulting in an annular eclipse. The penumbra, a broader surrounding region, produces partial obscuration as sunlight filters around the Moon's edges, spanning a much larger area on Earth, often thousands of kilometers wide. The occurrence and type of eclipse depend on the relative apparent angular diameters of the Sun and Moon as seen from Earth. The Sun's average angular diameter is approximately 0.53°, varying slightly between about 0.524° at aphelion and 0.542° at perihelion due to Earth's elliptical orbit. The Moon's angular diameter fluctuates more significantly, from roughly 0.49° at apogee (farthest point, ~406,000 km away) to 0.56° at perigee (closest point, ~363,000 km away), owing to its elliptical orbit. A total solar eclipse happens when the Moon's angular diameter is equal to or greater than the Sun's (), fully covering the solar disk; an annular eclipse occurs when , leaving a ring of sunlight visible. Parallax effects, arising from the observer's position on Earth's curved surface, introduce variations in the eclipse type along the shadow's path. For eclipses where the umbra's tip just grazes Earth's surface, the shadow may appear total at some locations due to the slight shift in the Moon's apparent position relative to the Sun (lunar parallax of about 1°), but annular at others where the curvature alters the line of sight. This results in hybrid eclipses, transitioning between total and annular phases over distances of tens to hundreds of kilometers. Solar eclipses require near-perfect alignment near the lunar nodes, which themselves regress westward along the ecliptic at a rate completing a full cycle every 18.6 years due to gravitational perturbations from the Sun. This nodal regression shifts the timing and location of eclipse seasons, ensuring that alignments for eclipses recur periodically but not at fixed calendar dates. Without this dynamic geometry, the slight orbital tilt would prevent the Moon from ever aligning closely enough with the ecliptic to cast its shadow on Earth during new moon phases.Prediction and Cycles
Calculation methods
The prediction of solar eclipses has evolved from empirical cycle-based methods to precise computational algorithms grounded in celestial mechanics. Ancient Babylonians, around 600 BCE, developed early predictive techniques by analyzing historical eclipse records on clay tablets spanning 609–447 BCE, identifying recurring patterns such as the Saros cycle of approximately 6,585 days (about 18 years), which allowed them to forecast similar eclipse geometries.[14] These arithmetic schemes enabled numerical predictions of the Moon's position without geometric models, achieving reasonable accuracy for their era.[15] A pivotal advancement occurred in 1715 when Edmond Halley produced the first modern prediction of a total solar eclipse visible over London on April 22, using Isaac Newton's laws of gravity and orbital mechanics from the Principia to calculate the event's timing and path with an accuracy of four minutes and 20 miles.[16] Halley integrated the ancient Saros cycle with Newtonian principles, publishing a map that encouraged systematic observations of totality duration.[14] Modern computations rely on high-precision ephemerides to determine the positions of the Sun, Moon, and Earth. The VSOP87 theory, developed by P. Bretagnon and G. Francou in 1986 at the Bureau des Longitudes, provides the Sun's ecliptic coordinates using a series of periodic terms referenced to the mean equinox of date.[17] For the Moon, the ELP2000/82 theory by M. Chapront-Touze and J. Chapront (1983) incorporates 37,862 terms for longitude, latitude, and distance, with mean errors of about 0.0006 seconds in right ascension and 0.006 arcseconds in declination, enabling eclipse phase timing predictions accurate to roughly 1/40 of a second.[17] These ephemerides form the basis for solving orbital equations derived from Kepler's laws to compute precise positions over millennia.[18] Algorithms then derive eclipse parameters from these positions, including gamma—the minimum distance of the Moon's shadow axis from Earth's center, measured in Earth equatorial radii—and the eclipse magnitude, defined as the fraction of the Sun's diameter obscured by the Moon at greatest eclipse.[19] Duration and path details are calculated using the geometry of the shadow cone, accounting for the Moon's radius (typically k=0.272281 for umbral contacts) and Earth's oblateness, to determine contact times and totality length along the central path.[18] Besselian elements, a set of time-dependent parameters introduced in the 19th century by Friedrich Bessel, further facilitate these calculations by parameterizing the eclipse path's orientation, curvature, and width for specific events.[15] Specialized software implements these methods for global predictions. NASA's Eclipse Predictions catalog, maintained by the Goddard Space Flight Center, uses VSOP87/ELP2000-85 ephemerides and algorithms from sources like Meeus (1982) to generate circumstances for eclipses from -1999 to +3000, including path widths and central durations.[18] The Institut de Mécanique Céleste et de Calcul des Éphémérides (IMCCE) in Paris provides complementary ephemerides and visibility maps, building on historical data to support observations of events like the 1999 August 11 eclipse.[15] Such predictions are highly reliable centuries in advance, with timing errors typically under a few seconds and path deviations up to 10 kilometers for near-term events, though uncertainties grow for distant futures due to variations in Earth's rotation (ΔT).[20] Post-1800 calculations benefit from refined historical rotation data, minimizing errors to fractions of a second.[20] Path calculations identify key points, such as the greatest eclipse—the instant when the shadow axis passes closest to Earth's center—and the greatest duration, where totality reaches its maximum along the path, often differing by 1–2 seconds and hundreds of kilometers.[21] The longest possible totality duration is approximately 7.5 minutes, limited by the Moon's shadow cone geometry at perigee.[21]Occurrence patterns
Solar eclipses occur between two and five times annually, with an average of approximately 2.38 per year over long periods, due to the alignment of the Moon's orbit with Earth's two eclipse seasons each year.[22] Each eclipse season spans about 34.5 days and can produce one or two eclipses, depending on the precise positions of the Sun, Earth, and Moon.[23] Over a 5,000-year span from 2000 BCE to 3000 CE, Earth experiences 11,898 solar eclipses, with roughly 35% being partial and 65% central (including total, annular, and hybrid types).[22] The recurrence of solar eclipses follows predictable cycles driven by the Moon's orbital parameters relative to the Sun and Earth's orbit. The Saros cycle, lasting 18 years, 11 days, and 8 hours (approximately 223 synodic months or 6,585.3 days), causes eclipses of the same type to repeat with similar characteristics, though the path on Earth shifts westward by about 120 degrees longitude each cycle due to the extra fractional day.[24] Each Saros series comprises 69 to 87 eclipses over 1,226 to 1,551 years, starting and ending with partial eclipses at high latitudes before transitioning to central ones near the equator.[23] Longer cycles refine these patterns further. The Inex cycle, spanning 10,571 days (about 29 years minus 20 days or 358 synodic months), integrates the Saros with the draconic year (the time for the Moon's nodes to return to the same position relative to the Sun, approximately 346.62 days), resulting in gradual shifts in eclipse latitude and a progression through the seasons.[25] Meanwhile, the Metonic cycle of 19 years (235 synodic months) ensures that lunar phases, including new moons conducive to eclipses, recur at nearly the same calendar date, aiding in seasonal alignment of eclipse occurrences.[23] Over geological timescales, the frequency and type of central eclipses will evolve as the Moon recedes from Earth at a rate of 3.8 cm per year, gradually reducing the Moon's apparent angular size relative to the Sun.[26] This recession, measured via lunar laser ranging, implies that total solar eclipses will cease in about 600 million years, after which all central eclipses will become annular.[27] Solar eclipses exhibit a global distribution influenced by the inclination of the Moon's orbit to the ecliptic. Central eclipses (total, annular, hybrid) are more frequent near the equator, where the umbral or antumbral path is widest, occurring roughly once every few years at low latitudes.[28] In contrast, polar regions primarily experience partial eclipses, as the narrower penumbral shadow limits central visibility, though annular eclipses appear more often at high latitudes due to the geometry of the Moon's apparent path.[28] This equatorial bias arises because the Moon's nodes, where eclipses can occur, align more readily with the Sun's position over tropical regions.[29]Observation and Viewing
Safety and partial viewing
Viewing the Sun during a partial or annular solar eclipse poses significant risks to eye health, as direct exposure can cause solar retinopathy, leading to retinal burns, blurred vision, or permanent blindness within seconds, even when the Sun appears partially obscured.[5] The intense ultraviolet and infrared radiation from the Sun's disk overwhelms the retina without warning, and there is no safe duration for unprotected viewing during these non-total phases.[30] Children and those with pre-existing eye conditions are particularly vulnerable to such damage.[31] Safe observation requires specialized equipment to filter out harmful wavelengths. The most accessible direct method uses eclipse glasses or handheld viewers certified to the ISO 12312-2 standard, which block at least 99.999% of visible light and nearly all UV and IR radiation; these must be inspected for scratches or tears before use and are suitable only for unaided eyes, not optical devices.[5] Indirect viewing via pinhole projectors offers a risk-free alternative: a small hole (about 1 mm) in an opaque card projects the Sun's crescent image onto a shaded surface, such as white paper inside a cardboard box, allowing group observation without eye strain.[5] No. 14 welder's glass, which meets or exceeds ISO standards for solar filtering, can also be used directly but must be the genuine shade 14 variant, as lower shades provide insufficient protection.[32] Partial solar eclipses, where the Moon covers only part of the Sun, are visible across vast regions, often spanning entire continents, with obscuration ranging from a few percent near the edges of the visibility zone to over 90% closer to the path of maximum eclipse, creating a noticeable crescent shape when more than 50% is obscured.[33] Unlike total eclipses, no point experiences complete coverage, so protective filters are mandatory throughout the event, and the dimming effect may subtly alter the environment, such as casting crescent-shaped shadows through tree leaves or colanders.[33] In total solar eclipses, the partial phases of ingress and egress last approximately 1 to 1.5 hours each, during which the Sun gradually emerges from behind the Moon at an angular velocity of about 0.5 degrees per hour, significantly slower than the Sun's emergence during sunrise, where the full disk appears in about 2–3 minutes at the equator due to Earth's rotational speed of 15 degrees per hour. This slow process emphasizes the need for prolonged safe viewing precautions throughout the entire event.[34][10] For annular eclipses, where the Moon appears smaller and leaves a bright ring of sunlight visible around its edge, the central filter must remain in place at all times, as the uneclipsed annular phase delivers nearly full solar intensity and can cause immediate retinal injury without protection.[30] The "ring of fire" effect, while striking, does not reduce the Sun's brightness enough for safe naked-eye viewing, requiring the same ISO-compliant filters as partial phases.[6] Accessibility is enhanced by digital tools, including NASA's Eclipse Explorer interactive map, which provides location-specific timings, obscuration percentages, and visibility paths for global planning. Mobile apps like those from Time and Date or the American Astronomical Society offer real-time alerts, countdowns, and augmented reality overlays to track the eclipse's progress without risking direct glances.[35] Authoritative bodies issue strict guidelines to prevent injuries: NASA warns against using unverified filters, binoculars, or cameras without dedicated solar attachments, emphasizing supervision for children and immediate medical attention for eye discomfort post-viewing.[5] The European Space Agency (ESA) similarly advises EU-certified protective eyewear and promotes projection methods, noting that even brief exposures during partial phases can lead to irreversible harm.[31] During significant partial obscuration (over 50%), animals may exhibit mild behavioral shifts, such as birds quieting or insects chirping earlier, reflecting the temporary twilight-like conditions.[33]Totality experience
As the Moon's shadow approaches the path of totality, the sky begins to darken noticeably about 10 to 15 minutes prior to the onset of totality, creating an eerie twilight effect even in midday. This gradual dimming intensifies, and observers often witness a surreal 360-degree sunset, where the horizon glows with orange and red hues all around due to sunlight illuminating the atmosphere beyond the shadow.[10] Concurrently, the air temperature typically drops by 5 to 10°C (9 to 18°F), with greater reductions possible in dry conditions, as the blockage of solar radiation reduces incoming heat.[36] During totality itself, which lasts from a few seconds up to a maximum of about 7 minutes and 32 seconds depending on the eclipse's geometry, the Sun's disk is completely obscured, allowing the naked eye to safely view the Sun's ethereal corona—a pearly white halo of plasma streams extending millions of kilometers into space.[10][37] This is the only natural circumstance in which the corona becomes visible without specialized equipment, as its faint glow is otherwise overwhelmed by the Sun's brilliant photosphere. Reddish solar prominences, loops of hot plasma erupting from the Sun's surface, may also appear along the limb, while brighter celestial objects like planets (e.g., Venus) and stars (e.g., Regulus) emerge against the darkened sky. The transition into and out of totality is marked by Baily's beads—brief flashes of sunlight piercing through lunar valleys—and the dramatic diamond ring effect, where a single bright point of light remains visible just before or after full coverage.[10] Following totality, the Sun emerges from behind the Moon during the egress partial phase, but this reappearance occurs much more slowly than the Sun's rising at sunrise. The relative angular velocity of the Moon with respect to the Sun is approximately 0.5 degrees per hour, resulting in the partial phases lasting about 1 to 1.5 hours as the Moon gradually uncovers the solar disk. In contrast, the apparent motion of the Sun at sunrise is due to Earth's rotation, which is about 15 degrees per hour, allowing the Sun's disk (approximately 0.53 degrees in diameter) to fully emerge above the horizon in roughly 2 to 3 minutes at equatorial latitudes. Consequently, the emergence during an eclipse is geometrically 30 to 40 times slower than at sunrise.[34][10] The sudden darkness profoundly affects the local environment and elicits strong emotional responses from viewers, often described as an overwhelming sense of awe or an "eclipse high" due to the surreal beauty and rarity of the event. Animals exhibit disoriented behaviors mimicking dusk or dawn: birds typically fall silent and may roost, while nocturnal insects like crickets begin chirping. Clear skies are essential for unobstructed viewing, though cloud cover frequently obstructs totality along the path, underscoring the role of weather in the overall experience.[10][38]Advanced techniques
Eclipse chasing refers to the pursuit of optimal viewing conditions for total solar eclipses by dedicated enthusiasts and professionals who travel globally to intercept the path of totality. Organized tours, often led by astronomical societies or specialized operators, facilitate access to remote sites with coordinated logistics, including transportation and on-site support.[39] Weather forecasting plays a critical role, with chasers relying on advanced cloud models and climatological data to predict clear skies along the eclipse track, such as those analyzed for the 2024 North American eclipse using long-range models from sources like NOAA.[40] Prominent chasers like Glenn Schneider, an astronomer at the University of Arizona, successfully navigated multiple eclipses by combining precise path calculations with real-time weather adjustments, as demonstrated in his intercepts during the 2003 total eclipse in Antarctica.[39] Advanced photography of solar eclipses requires specialized equipment to capture the corona and surrounding phenomena safely and effectively. Solar telescopes, such as the Coronado 60mm SolarMax II, equipped with H-alpha filters, allow imaging of the chromosphere and prominences during partial phases by isolating the hydrogen-alpha emission line at 656.3 nm.[41] For totality, wide-field techniques using a standard 50mm lens on a DSLR camera capture the darkened sky and foreground landscape, while telephoto setups with 500–2,000mm focal lengths enable detailed corona shots through timed exposures—short bursts under 1 second for bright inner corona features and longer ones up to several seconds for faint outer streamers—often bracketed to handle the wide dynamic range.[42] Stable mounts, like equatorial trackers, minimize vibrations, and RAW format recording preserves data for post-processing.[42] Precise timing is essential for maximizing totality, with alerts for second contact (the start of totality) and third contact (its end) provided by apps and software that warn observers seconds in advance to prepare equipment. GPS devices enhance path accuracy to within ±100 meters, crucial for edge-of-path viewing where totality duration can vary by seconds, as seen in validations during the 2017 U.S. eclipse.[43][44] From space, solar eclipses offer a unique perspective, as observed by astronauts on the International Space Station (ISS), which orbits at 250 miles altitude and avoids Earth's umbral shadow due to its position above the atmosphere. Crew members have captured the Moon's dark disk transiting the Sun or the umbra racing across Earth's surface, as during the 2024 eclipse when the ISS crossed the path three times.[45][46] Amateur data collection during eclipses includes spectroscopy to study the chromosphere, using slit-less spectrographs attached to telescopes to produce the "flash spectrum"—a brief rainbow of emission lines visible only at second and third contacts, revealing elements like hydrogen and helium. Equipment such as compact spectrometers or modified cameras with diffraction gratings allows enthusiasts to record these spectra for analysis of solar activity.[47] Logistics for remote eclipse paths often involve charter flights to inaccessible regions like the Arctic or Antarctic, where operators provide specialized transport such as flights from Punta Arenas, Chile, to Union Glacier in Antarctica, lasting about 4.25 hours. These expeditions incur high costs, typically $10,000–$25,000 per person (as of 2025) for fly-cruise packages, covering fuel surcharges, polar gear, and contingency planning for variable ice conditions.[48][49][50]Historical and Scientific Context
Notable historical eclipses
One of the earliest recorded solar eclipses appears in Chinese annals from the Book of Documents (Shu Ching), dated to October 22, 2137 BCE, during the Xia dynasty, where two court astronomers, Hsi and Ho, were reportedly executed for failing to predict the event.[51] Modern astronomical calculations confirm the visibility of a total solar eclipse in ancient China on that date, validating the historical record as the oldest documented observation of such a phenomenon.[52] In ancient Mesopotamia, Assyrian scribes documented a total solar eclipse on June 15, 763 BCE, in the eponym canon from Nineveh, noting it alongside civil unrest in the region.[53] This eclipse, visible over northern Assyria, is one of the earliest precisely dated astronomical events in cuneiform records and may have influenced biblical chronology, as referenced in the Book of Amos.[54] The solar eclipse of May 28, 585 BCE, holds particular historical significance due to its purported prediction by the Greek philosopher Thales of Miletus, who used geometric principles to forecast the event based on Babylonian eclipse cycles.[55] According to Herodotus, the eclipse interrupted a battle between the Lydians and Medes, prompting both sides to cease fighting and negotiate peace under the darkened sky.[56] This event marked an early milestone in predictive astronomy and underscored eclipses' role in ancient diplomacy. Solar eclipses profoundly shaped cultural narratives across civilizations. In ancient China, eclipses were mythologized as a celestial dragon devouring the sun, prompting rituals of banging drums and pots to scare the beast away and restore light; such beliefs persisted alongside meticulous records in imperial annals.[57] Similarly, the Maya integrated eclipse predictions into their 260-day ritual calendar (Tzolk'in), viewing them as cosmic battles where the sun god Kinich Ahau clashed with underworld forces, often portending drought, war, or societal upheaval, as evidenced in codices and stelae alignments.[58] During the medieval period, a total solar eclipse on May 5, 840 CE, visible across Europe, was interpreted as a dire omen by Carolingian observers, occurring shortly before the death of Louis the Pious, son of Charlemagne, and fueling superstitions about celestial signs heralding royal demise.[59] In the Islamic world, detailed accounts of a solar eclipse on September 13, 1178 CE, appear in chronicles by Ibn al-Jawzi and al-Tabari, describing its path and timing with precision that aided later astronomical verification.[60] The total solar eclipse of June 8, 1918, crossed the continental United States from Oregon to Florida, drawing widespread public interest and scientific observation, with a maximum totality duration of 2 minutes 37 seconds in parts of the path.[61] Just a year later, the May 29, 1919, eclipse prompted expeditions led by Arthur Eddington to Príncipe and Sobral, Brazil, where measurements of starlight deflection by the sun's gravity confirmed Einstein's general theory of relativity, revolutionizing physics.[62] In a milestone for media coverage, the total solar eclipse of March 7, 1970, which traversed the Pacific Ocean before sweeping across North America from the Pacific Northwest to Virginia, became the first to be broadcast live on television by CBS in color, allowing millions to witness totality remotely.[63]Scientific observations and phenomena
One of the most significant scientific observations during a solar eclipse occurred on May 29, 1919, when expeditions led by Arthur Eddington and Frank Watson Dyson measured the deflection of starlight by the Sun's gravitational field, confirming Albert Einstein's general theory of relativity. Observations from Príncipe and Sobral, Brazil, revealed a mean deflection of 1.75 arcseconds for stars near the Sun, closely matching Einstein's predicted value of 1.75 arcseconds, as opposed to the 0.87 arcseconds expected under Newtonian gravity; the results were published by Dyson, Eddington, and Charles R. Davidson in the Philosophical Transactions of the Royal Society.[64] Solar eclipses provide a unique opportunity to study the Sun's corona, the outermost layer of the solar atmosphere, which is otherwise obscured by the photosphere's brightness. The corona consists primarily of plasma at temperatures ranging from 1 to 2 million Kelvin, far hotter than the Sun's surface, and serves as the origin of the solar wind, a stream of charged particles that permeates the heliosphere. Spectroscopic analyses during eclipses have identified its composition as highly ionized gases, including helium, oxygen, and iron, with elemental abundances that trace solar wind fractionation processes.[65] Several distinctive phenomena are observable just before and after totality. Shadow bands, fleeting wavy patterns of light and dark on the ground, result from atmospheric turbulence refracting the thin crescent of sunlight near second and third contact, with turbulence primarily occurring below 2 kilometers altitude. The green flash, a brief burst of green light at second contact, arises from atmospheric refraction separating the Sun's rays by wavelength, with shorter green wavelengths bending more than red, creating a momentary emerald rim on the lunar edge.[66] Eclipses have revealed anomalies in physical and biological systems. Gravimeters have detected subtle gravity variations during totality, on the order of microgals, potentially linked to microseisms or atmospheric gravity waves induced by rapid cooling, though some reports suggest unexplained anomalies requiring further verification.[67] Studies of animal behavior indicate disorientation, with diurnal species like birds ceasing calls and nocturnal ones activating prematurely; for instance, during the 2017 eclipse, zoo animals across 17 species exhibited evening-like routines, such as gorillas returning to enclosures.[68] While solar eclipses allow direct measurement of the Sun's angular diameter, transits of Venus and Mercury provide complementary data for determining the solar radius, as the planets' known sizes and paths across the disk enable precise calibration without atmospheric distortion during eclipses. For example, observations of Mercury's 10-arcsecond disk against the Sun's 1900-arcsecond diameter during May transits have refined solar scale estimates. Eclipses induce ionospheric disturbances by reducing solar ionizing radiation, leading to recombination in the D-layer and temporary radio blackouts on high-frequency bands, with signal absorption increasing by up to 20 dB during totality.[70] Satellite operations, including GPS, experience glitches from these ionospheric scintillations and thermal effects on geostationary spacecraft, causing positioning errors of several meters, as observed during the 2017 eclipse.[71] Modern research leverages space-based instruments like the Solar and Heliospheric Observatory (SOHO) and Solar Terrestrial Relations Observatory (STEREO) to complement ground-based eclipse data, capturing coronal mass ejections and streamer structures in white light without atmospheric interference.[72] Citizen science initiatives, such as GLOBE Observer and Eclipse Soundscapes apps, have collected millions of observations during recent eclipses, contributing to databases on atmospheric and acoustic effects.[73] Post-2020 studies, including analyses of the April 8, 2024, total eclipse, have examined correlations with ozone dynamics, finding minimal total column ozone variations (less than 1.2 Dobson Units) attributable to reduced photolysis, though short-term stratospheric cooling may influence local ozone profiles amid broader climate interactions.[74]Modern and Future Eclipses
Recent events
The total solar eclipse of August 21, 2017, crossed the United States from coast to coast, beginning in Oregon and ending in South Carolina, with a maximum duration of totality of 2 minutes and 40 seconds.[75] This event was visible across much of North America, drawing widespread public interest and scientific observation.[75] On July 2, 2019, another total solar eclipse occurred, with its path of totality passing over the South Pacific Ocean, Chile, and Argentina, achieving a maximum duration of 4 minutes and 33 seconds.[75] The eclipse was visible primarily in southern South America and surrounding oceanic regions.[75] The annular solar eclipse of June 21, 2020, traversed central Africa, southern Asia, and parts of China, with a central duration of 38 seconds and a maximum eclipse magnitude of 0.994.[75] It was observable across Africa, southeastern Europe, and Asia.[75] An annular eclipse took place on June 10, 2021, affecting northern Canada, Greenland, and extreme northeastern Russia, with a central duration of 3 minutes and 51 seconds.[76] Visibility extended to northern North America, Europe, and Asia.[76] The partial solar eclipse of October 25, 2022, was visible in Europe, northeastern Africa, the Middle East, and western Asia.[76] On October 14, 2023, an annular solar eclipse crossed the Americas, including the western United States, Central America, Colombia, and Brazil, featuring a central duration of 5 minutes and 17 seconds.[76] It was widely seen across North, Central, and South America.[76] The total solar eclipse of April 8, 2024, followed a path through Mexico, central United States, and eastern Canada, with a maximum totality duration of 4 minutes and 28 seconds.[76] This event attracted the largest audience of any recent U.S. eclipse, with approximately 32 million people residing along the path of totality.[77] It generated significant economic impacts, including an estimated $6 billion boost to the U.S. economy from tourism, travel, and related spending, alongside increased traffic volumes in affected regions.[78][79] An annular eclipse occurred on October 2, 2024, visible in the South Pacific, southern Chile, and southern Argentina, with a central duration of 7 minutes and 25 seconds.[76] The partial solar eclipse of March 29, 2025, was observed in northwestern Africa, Europe, North America, and northern Russia.[76] The partial solar eclipse of September 21, 2025, was visible in New Zealand, eastern Australia, the southern Pacific Ocean, and parts of Antarctica.[76]Forthcoming eclipses
Earlier in 2026, an annular solar eclipse on February 17, 2026, will cross southern Argentina, southern Africa, and Antarctica, featuring a maximum annularity of 2 minutes and 20 seconds.[76] The next total solar eclipse will occur on August 12, 2026, visible across a path from northern Greenland through Iceland and into Spain, with a maximum duration of totality of 2 minutes and 18 seconds near the center of the path in the Atlantic Ocean off Iceland's coast.[76] Partial phases will be observable over much of Europe, northern Africa, and parts of North America. In 2027, a total solar eclipse on August 2 will traverse North Africa and southern Europe, including Morocco, Spain, and extending to the Arabian Peninsula and Somalia, offering the longest duration of totality among eclipses until 2126 at 6 minutes and 23 seconds near Luxor, Egypt.[76] An earlier annular event on February 6, 2027, will be visible over Chile, Argentina, and the southern Atlantic, with annularity lasting up to 7 minutes and 51 seconds.[76] The year 2028 features an annular eclipse on January 26 over Ecuador, Peru, Brazil, and parts of southern Europe, achieving a record annularity of 10 minutes and 27 seconds for the decade off the coast of Brazil.[76] Later that year, a total eclipse on July 22 will sweep across Australia and New Zealand, with totality up to 5 minutes and 10 seconds in southeastern Australia.[76] Advancing to 2029 and 2030, all solar eclipses will be partial except for central events in 2030: an annular eclipse on June 1 visible from Algeria through Turkey, Russia, China, and Japan, with 5 minutes and 21 seconds of annularity; and a total eclipse on November 25 crossing Botswana, South Africa, and Australia, lasting up to 3 minutes and 44 seconds in the Indian Ocean.[76] These predictions, derived from orbital ephemerides, remain stable as of 2025, unaffected by short-term environmental factors, though long-term climate shifts may subtly alter local weather patterns and visibility conditions along paths.[80]| Date | Type | Maximum Duration | Primary Path of Visibility |
|---|---|---|---|
| 2026 Feb 17 | Annular | 2m 20s | Southern Argentina, southern Africa, Antarctica |
| 2026 Aug 12 | Total | 2m 18s | Greenland, Iceland, Spain |
| 2027 Feb 6 | Annular | 7m 51s | Chile, Argentina, southern Atlantic |
| 2027 Aug 2 | Total | 6m 23s | Morocco, Spain, Arabian Peninsula, Somalia |
| 2028 Jan 26 | Annular | 10m 27s | Ecuador, Peru, Brazil, southern Europe |
| 2028 Jul 22 | Total | 5m 10s | Australia, New Zealand |
| 2030 Jun 1 | Annular | 5m 21s | Algeria, Turkey, Russia, China, Japan |
| 2030 Nov 25 | Total | 3m 44s | Botswana, South Africa, Australia |
References
- https://eclipse.gsfc.[nasa](/page/NASA).gov/transit/catalog/MercuryCatalog.html