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sun

  (sŭn) pronunciation
sun
(Click to enlarge)
sun
cutaway of the sun
(Academy Artworks)
n.
  1. often Sun A star that is the basis of the solar system and that sustains life on Earth, being the source of heat and light. It has a mean distance from Earth of about 150 million kilometers (93 million miles) a diameter of approximately 1,390,000 kilometers (864,000 miles) and a mass about 330,000 times that of Earth.
  2. A star that is the center of a planetary system.
  3. The radiant energy, especially heat and visible light, emitted by the sun; sunshine.
  4. A sunlike object, representation, or design.

v., sunned, sun·ning, suns.

v.tr.

To expose to the sun's rays, as for warming, drying, or tanning.

v.intr.

To expose oneself or itself to the sun.

idioms:

in the sun

  1. In the public eye.
under the sun
  1. On the earth; in the world.

[Middle English, from Old English sunne.]


 
 

The star around which the Earth revolves, and the planet's source of light and heat, hence life. The Sun is a globe of gas, 1.4 × 106 km (8.65 × 105 mi) in diameter with a mass 333,000 times the Earth, held together by its own gravity. The surface temperature of the Sun is about 6000 K (10,000°F); since solids and liquids do not exist at these temperatures, the Sun is entirely gaseous. Almost all the gas is in atomic form, although a few molecules exist in the coolest surface regions, such as sunspots.

The Sun is a typical member of the spectral class dG2, stars of surface temperature 6000 K. The d stands for a dwarf, a normal star of that class. See also Spectral type.

Solar structure

The interior of the Sun can be studied only by inference from the observed properties of the entire star. The great mass of the Sun presses down on the center, requiring a gas with a central density of near 90 g/cm3 and 2 × 107 K (3.6 × 106°F) temperature to support it. At these huge temperatures and densities, nuclear reactions take place. The radiation produced flows outward till it is radiated into space by the surface (photosphere) at 6000 K (10,000°F).

Energy production

The energy of the Sun is produced by the conversion of hydrogen into helium. For each hydrogen atom converted, one neutrino is produced. These neutrinos are detected, but less than the expected number. See also Neutrino; Solar neutrinos.

The material at the center of the Sun is so dense that a few millimeters are opaque, so the photons created by nuclear reactions are continually absorbed and reemitted and thus make their way to the surface by a random walk. The atoms in the center of the Sun are entirely stripped of their electrons by the high temperatures, and most of the absorption is by continuum processes, such as the scattering of light by electrons. Because there are so many absorption and emission processes along the way, it can take as long as a million years to complete the random walk to the surface.

Convection

In the outer regions of the solar interior, the temperature is low enough for ions and even neutral atoms to form and, as a result, atomic absorption becomes very important. The high opacity makes it very difficult for the radiation to continue outward, so steep temperature gradients are established that result in convective currents. Most of the outer envelope of the Sun is in such convective equilibrium. These large-scale mass motions are responsible for the complex phenomena observed at the surface. See also Convection (heat).

Radiation

Electromagnetic energy is produced by the Sun in essentially all wavelengths. However, more than 95% of the energy is concentrated in the relatively narrow band between 290 and 2500 nm and is accessible to routine observation from ground stations on Earth. The maximum radiation is in the green region, and the eyes of human beings have naturally evolved to be sensitive to this range of the spectrum. The total radiation is called the solar constant. It is not exactly constant but varies slightly (±0.1%) with the solar cycle. The ultraviolet flux, however, varies by substantial factors depending on the exact wavelength, and this affects the Earth's upper atmosphere. See also Electromagnetic radiation; Solar constant.

Atmosphere

Although the Sun is gaseous, it can be seen only to the point at which the density is so high that the material is opaque. This layer, the visible surface of the Sun, is termed the photosphere. Light from father down reaches the Earth by repeated absorption and emission by the atoms, but the deepest layers cannot be seen directly. The surface is actually not sharp, but the Sun is so far away that the smallest distance that can be resolved with the best telescope is about 300 km (200 mi). Since the density e-folding height (scale height) is less than 200 km (120 mi), the edge appears sharp. See also Photosphere.

Above the photosphere the atmosphere is transparent, and its density falls off much more slowly because magnetic fields support the ionized particles. The atmosphere can be seen by using a narrow-band filter or a spectrograph to pick out the isolated wavelengths absorbed by the atmospheric gases. In the upper photosphere it is cooler, and the lines are dark. If the light is imaged in the strongest lines, such as those of hydrogen, a region higher still is seen, called the chromosphere. The light from this region is dominated by the red hydrogen alpha (level 2 → 3 transition) line, which gives it a rosy color seen at a solar eclipse. The chromosphere is a rapidly fluctuating region of jets and waves coming up from the surface. When all the convected energy coming up from below reaches the surface, it is concentrated in the thin material and produces considerable activity. Where the magnetic field is stronger, these waves are absorbed, and raise the temperature to 7000–8000 K (12,000–14,000°F). The scale height of the chromosphere is 1000 km (600 mi) or more, so there no longer is a sharp edge. See also Chromosphere; Eclipse.

When the Moon obscures the Sun at a total solar eclipse, the vast extended atmosphere of the Sun called the corona can be seen. The corona is a million times fainter than the photosphere, so it is visible only when seen against the dark sky of an eclipse or with very special instruments. Its density is low, but its temperature is high (more than 106 K or 1.8 × 106°F). The hot gas evaporating out from the corona flows steadily to the Earth and farther in the solar wind. See also Solar corona; Solar wind.

Coronal holes

Early coronal observations showed that the corona was occasionally absent over certain regions. In particular, at sunspot minimum it was quite weak over the poles. X-ray pictures revealed great bands of the solar surface essentially devoid of corona for many months. These proved to be regions where the local magnetic fields were connected to quite distant places, so the fields actually reached out to heights from which the solar wind could sweep the gas outward. Analysis of solar wind data showed that equatorial coronal holes were associated with high-velocity streams in the solar wind, and recurrent geomagnetic storms were associated with the return of these holes. Thus the relative intensity of the corona over sunspot regions is partly due to their strong, closed magnetic fields which trap the coronal gas.

Solar activity

There are a number of transient phenomena known collectively as solar activity. These are all connected with sunspots.

Sunspots

Sunspots were discovered around 1610. Heinrich Schwabe announced in 1843 that their number rose and fell with a 10-year period. Subsequent study of the old records revealed an 11-year period since the original discovery.

The number of sunspots peaks soon after the beginning of each cycle and decays to a minimum in 11 years. The first spots of a number cycle always occur at higher latitudes, between 20° and 35°, and the latitude of occurrence decreases as the cycle unfolds (Spörer's law). Almost no spots are observed outside the latitude range of 5–35°. The great majority are small and last a few days, but some last for two rotations. In 1908, George Ellery Hale discovered that sunspots had strong magnetic fields. Each spot group contains positive and negative magnetic polarity (monopoles are forbidden by Maxwell's laws). Hale found that the polarities were mirrored, with the same polarity generally leading in one hemisphere and following in the other. He found that with each new number cycle the lead polarity switches, so that the complete magnetic cycle lasts 22 years. But each new number cycle starts a few years before the end of the previous one, so the average duration of a half-cycle is nearly 14 years. See also Magnetism.

The darkness of sunspots ( Fig. 1) is probably due to the intense magnetic fields (3000 gauss or 0.3 tesla), which cool the surface by suppressing the normal convective energy flow from below. It takes several days for the darkening to occur.

Large symmetric sunspot photographed in Hα light. Clock indicates time of photograph. (<i>Big Bear Solar Observatory</i>)
Large symmetric sunspot photographed in Hα light. Clock indicates time of photograph. (Big Bear Solar Observatory)

Although the sunspot is cool, its neighborhood is the scene of the hottest and most intense activity, generally referred to as an active region. Magnetic energy is continually released there. The corona above an active region is hot and dense, roughly three times hotter and denser than in quiet regions.

Prominences

The term “prominence” is used for any cloud of cool gas in the corona, where it appears bright against the sky. Because these clouds absorb the chromospheric light and scatter it, they appear dark against the solar disk in Hα and other strong lines. In continuous light they are transparent. At the limb we see the chromospheric light they scatter against the dark sky. Since they are much denser than the corona, something must hold them up against gravity. Prominences are found only in regions of horizontal magnetic fields that support them. Thus filaments on the disk, which may last for weeks, are good markers of the magnetic boundaries. When the magnetic structure changes, prominences become unstable and erupt, always upward. They also may be ejected by solar flares or appear as graceful loops raining from the corona after flares. Erupting prominences are probably the source of coronal mass ejections, in which a bubble of coronal material erupts outward at several hundred kilometers per second and flows out into interplanetary space.

Plages

Just as prominences occur when the magnetic field changes from one sign to the other, plages occur whenever the magnetic field is vertical and relatively strong but not strong enough to form a sunspot. They are bright regions in any strong spectrum line, because the chromosphere is heated there. In a typical active region, the preceding magnetic field is clumped in a sunspot and the following field spread out in a plage. In Hα light, the plage is seen to be connected to the sunspot by dark fibrils outlining the lines of force.

Flares

The most spectacular activity associated with sunspots is the solar flare ( Fig. 2). A flare is defined as an abrupt increase in the Hα emission from the sunspot region. The brightness of the flare may be up to eight times that of the chromosphere; the rise time is seldom longer than a few minutes. The Hα brightening results from heating of the chromosphere at the foot points of the magnetic field by a tremendous energy release in the atmosphere. While flares are usually visible only in chromospheric lines, the foot points of big flares can be seen in white light. From the foot points, a cloud of hot material, up to 3 × 107 K (5.4 × 107°F) arises and concentrates at the arch tops. This cloud condenses out in an array of loop prominences. An active sunspot group produces a hierarchy of flares, a few big and many small ones.

The great “sea horse” flare of August 7, 1972, late in the flare, photographed in the blue wing of the Hα line. The neutral line between two bright strands is crossed by an arcade of bright loop prominences raining down from the corona. (<i>Big Bear Solar Observatory</i>)
The great “sea horse” flare of August 7, 1972, late in the flare, photographed in the blue wing of the Hα line. The neutral line between two bright strands is crossed by an arcade of bright loop prominences raining down from the corona. (Big Bear Solar Observatory)

Flares are often associated with the eruption of filaments. A few minutes after the eruption begins, there is an abrupt acceleration and a storm of energetic particles is produced, heating the corona to flare brightness.

The flare produces a huge stream of solar energetic particles (SEP) as well as shock waves. A huge magnetohydrodynamic shock wave flies out at about 1000 km/s (600 mi/s) and continues into interplanetary space, often reaching the Earth. The wave produces a huge radio burst in the meter-wavelength range as it excites the coronal layers. The energetic nuclei produce gamma-ray lines from nuclear reactions as they penetrate to the photosphere. If they are sufficiently numerous, they heat the photosphere faster than it can reemit energy and a white light flare is observed, usually in the form of bright transient flashes at the foot points of the flare loops. The particles reach the Earth in a great particle storm.


 

(Sun Microsystems, Inc., Santa Clara, CA, www.sun.com. A major manufacturer of Unix-based workstations and servers. In 1981, Bavarian-born Andreas Bechtolsheim was licensing rights to a computer he designed. Named Sun for Stanford University Network and using off-the-shelf parts, it was an affordable workstation for engineers and scientists. In that year, he met Vinod Khosla, a native of India, who convinced him to form a company and expand. Khosla, Bechtolsheim and Scott McNealy, all Stanford MBAs, founded Sun in 1982.

Its first computers, the Sun-1 and subsequent Sun-2 were instant successes in the university market. Sun began to compete against its rival Apollo Computer, an east-coast workstation company, eventually surpassing it in sales (Apollo was later purchased by HP).

Sun has been a major force in open systems. Its computers have always run under Unix, which was licensed from AT&T and then later purchased outright. Sun and AT&T had formed such a tight alliance for a while that a host of Unix vendors formed the Open Software Foundation (OSF) in 1988 to keep Sun from dominating Unix.

In 1984, Bill Joy, head of R&D, designed NFS, which was broadly licensed and became the industry standard for file sharing. Sun later packaged its Unix components into a complete environment named Solaris, which it later ported to other platforms, including the Intel x86.

Sun used the Motorola 68K CPUs in its products until it designed its own RISC-based SPARC chips, which it launched with the SPARCstation 1 in 1989. Having gone through many iterations, SPARC CPUs are also made by Fujitsu and other third parties via licensing arrangements (see SPARC).

In the mid-1990s, Sun introduced the Java programming language and ushered in a new era for application development on the Internet (see Java and J2EE). Later on, Sun was a major proponent of network computers. See network computer and Sun-Netscape Alliance.

The Founders
From left to right: Vinod Khosla, Bill Joy, Andreas Bechtolsheim and Scott McNealy. Although Joy was not a founder, he was hired shortly thereafter and became one of Sun's major contributors.

The Sun-1
Sun's workstations were an instant success primarily in the university market. This led many professionals to the company who helped it grow steadily.

The First SPARCstation
In 1989, Sun introduced the SPARCstation 1, the first Sun computer that used the SPARC chip.

Sun JavaStation
Sun developed the Java programming language, and its network computer is aptly named. The JavaStation conforms to the NC Reference Profile and is available in several models.



 
Idioms: sun

Idioms beginning with sun:
sundry
sun belt

In addition to the idiom beginning with sun, also see everything but the kitchen sink (under the sun); make hay while the sun shines; nothing new under the sun; place in the sun.


 

Star around which the components of the solar system revolve. It is about five billion years old and is the dominant body of the system, with more than 99% of its mass. It converts five million tons of matter into energy every second by nuclear fusion reactions in its core, producing neutrinos (see solar neutrino problem) and solar radiation. The small amount of this energy that penetrates Earth’s atmosphere provides the light and heat that support life. A sphere of luminous gas 864,950 mi (1,392,000 km) in diameter, the Sun has about 330,000 times the mass of Earth. Its core temperature is close to 27 million °F (15 million °C) and its surface temperature about 10,000 °F (6,000 °C). The Sun, a spectral type G (yellow) star, has fairly average properties for a main-sequence star (see Hertzsprung-Russell diagram). It rotates at different rates at different latitudes; one rotation takes 36 days at the poles but only 25 days at the equator. The visible surface, or photosphere, is in constant motion, with the number and position of sunspots changing in a regular solar cycle. External phenomena include magnetic activity extending into the chromosphere and corona, solar flares, solar prominences, and the solar wind. Effects on Earth include auroras and disruption of radio communications and power-transmission lines. Despite its activity, the Sun appears to have remained relatively unchanged for billions of years. See also eclipse; heliopause.

For more information on Sun, visit Britannica.com.

 

One of the chief origin theories proposed by 19th-century scholars, especially Max Müller, was that numerous seasonal customs, from bonfires to cheese rolling, originally celebrated, encouraged, or mimicked the solar cycle. Arguments for the solar interpretation of fire festivals can be found in Frazer's Golden Bough, though on balance he thinks it likelier that they were designed to ward off evil.

Actual English folk beliefs concerning the sun are few. It was said to be lucky to dance at dawn on Easter Day, when people would climb hills in the hope of seeing this sight, or try to catch its reflection in pails of water. Occasionally, children were told it was wicked to point at the sun, and you could be struck dead for doing so. More commonly, women maintained that direct sunlight on the hearth would ‘put the fire out’, and would draw curtains or place screens to prevent this; this may have developed from a medieval idea that if a house was on fire, sunshine could extinguish the blaze (Opie and Tatem, 1989: 381).

See RIGHTWARD MOVEMENT.

 
intensely hot, self-luminous body of gases at the center of the solar system. Its gravitational attraction maintains the planets, comets, and other bodies of the solar system in their orbits.

General Characteristics of the Sun

The sun is actually a star of about medium size; it appears larger than the other stars because of its relative nearness to the earth. The earth's distance from the sun varies from 91,377,000 mi (147,053,000 km) at perihelion to 94,537,000 mi (152,138,000 km) at aphelion (see apsis). The mean distance is c.92,960,000 mi (149,591,000 km); this is taken as the astronomical unit (AU) of distance used for measuring distances within the solar system. The sun is approximately 865,400 mi (1,392,000 km) in diameter, and its volume is about 1,300,000 times that of the earth. Its mass is almost 700 times the total mass of all the bodies in the solar system and 332,000 times that of the earth. The sun's surface gravity is almost 28 times that of the earth; i.e., a body on the surface of the sun would weigh about 28 times its weight on earth. The density of the material composing the sun is about one fourth that of the earth; compared with water, the sun's average density is 1.41. At its center, the sun has a density of over 100 times that of water, a temperature of 10 to 20 million degrees Celsius, and a pressure of over 1 billion atmospheres.

Observations of sunspots and studies of the solar spectrum indicate that the sun rotates on its axis from east to west; because of its gaseous nature its rate of rotation varies somewhat with latitude, the speed being greatest (a period of almost 25 days) in the equatorial region and least at the poles (a period of about 35 days). The axis of the sun is inclined at an angle of about 7° to the plane of the ecliptic.

The bright surface of the sun is called the photosphere. Its temperature is about 6,000°C. The photosphere appears darker near the edge (limb) of the sun's disk because of greater absorption of light by the sun's atmosphere in this area; this phenomenon is called limb darkening. During an eclipse of the sun the chromosphere and the corona (the outer layers of the sun's atmosphere) are observed. Also of interest is the high-speed, tenuous extension of the corona known as the solar wind.

Production of Solar Energy

The vast and continual production of solar energy cannot be attributed merely to combustion, to the gradual cooling of a hot body, to the fall of meteorites into the sun, or to gradual shrinkage with transformation of potential energy into heat (a theory proposed by Helmholtz). The theory of relativity with its implication of the equivalence of mass and energy led to the assumption that energy stored in the atoms constituting the sun's gases is constantly being released by conversion of some of the masses of the atom's nuclei during nuclear transmutations (see nuclear energy). H. A. Bethe proposed a cycle of nuclear reactions known as the carbon cycle, or CNO bi-cycle, to account for the nuclear changes. In this cycle carbon acts much as a catalyst, while hydrogen is transformed by a series of reactions into helium and large amounts of high-energy gamma radiation are released. It is now thought that the so-called proton-proton process is a more important energy source; this process begins with the collision of two protons and ends with the production of helium, while gamma radiation is released throughout.

See nucleosynthesis; stellar evolution.

The Study of the Sun

By means of the spectroscope much has been learned about the composition of the sun. There are numerous dark lines of varying widths in the solar spectrum. These were first intensively studied by Joseph Fraunhofer and are commonly known by his name. From a study of the lines the chemical composition of the sun is determined on the basis of the discovery by Kirchhoff that the dark lines correspond in position to the bright lines characteristic of the spectra produced by elements in the laboratory. The darkness of the lines in the sun's spectrum is attributed to the presence of a slightly cooler layer of gases above the photosphere, known as the reversing layer, which absorbs selectively the light of the photosphere and thus causes dark lines instead of bright ones to be observed through the spectroscope. By comparison of the sun's spectrum with laboratory spectra of incandescent elements, most of the elements known on earth have been identified in the sun's atmosphere.

Beyond the red portion of the visible solar spectrum is the infrared spectrum; for the study of these heat rays S. P. Langley invented the bolometer, a highly sensitive electrical device for measuring temperature. Solar heat and energy are measured by an instrument called the pyrheliometer. Other instruments devised especially for the study of the sun are the coronagraph and the spectroheliograph. These instruments have revealed a number of interesting phenomena occurring during the periods of solar activity associated with sunspots, e.g., faculae, plages (flocculi), prominences, and flares.

Importance to Terrestrial Life

Without the heat and light of the sun, life as we know it could not exist on the earth. Since solar energy is used by green plants in the process of photosynthesis, the sun is the ultimate source of the energy stored both in food and fossil fuels. Solar heating sets up convection currents, and thus is the source of the energy of moving air. Falling rain also owes its energy to the sun because of the relation of solar radiation to the water cycle.

Bibliography

See K. Hufbauer, Exploring the Sun: Solar Science since Galileo (1993); R. Krippenhahn, Discovering the Secrets of the Sun (1994); K. J. H. Phillips, Guide to the Sun (1995); P. O. Taylor, Beginners Guide to the Sun (1996); S. T. Suess and B. T. Tsurutani, ed., From the Sun: Auroras, Magnetic Storms, Solar Flares, Cosmic Rays (1998).


 

The star around which the Earth revolves.

  • The sun is about 4.5 billion years old and is expected to remain in its present state for approximately another six billion years; it will eventually evolve into a white dwarf.
  •  
    pronunciation

    IN BRIEF: The planet that lights and heats the earth during the day. The star around which the earth revolves.

    pronunciation We moved our blanket under a tree to get out of the sun.

     

    Quotes:

    "The sun was like a great visiting presence that stimulated and took its due from all animal energy. When it flung wide its cloak and stepped down over the edge of the fields at evening, it left behind it a spent and exhausted world." - Willa Cather

    "The Sun, the hearth of affection and life, pours burning love on the delighted earth." - Arthur Rimbaud

    "The day of the sun is like the day of a king. It is a promenade in the morning, a sitting on the throne at noon, a pageant in the evening." - Wallace Stevens

    "The sun is but a morning star." - Henry David Thoreau

    "Nobody of any real culture, for instance, ever talks nowadays about the beauty of sunset. Sunsets are quite old fashioned. To admire them is a distinct sign of provincialism of temperament. Upon the other hand they go on." - Oscar Wilde

     
    The Sun Sun_symbol.svg
    The Sun
    Observation data
    Mean distance
    from Earth
    1.496×1011 m
    8.31 min at light speed
    Visual brightness (V) −26.74m [54]
    Absolute magnitude 4.83m [54]
    Spectral classification G2V
    Angular size 31.6' - 32.7' [55]
    Adjectives solar
    Orbital characteristics
    Mean distance
    from Milky Way core
    ~2.5×1020 m
    26,000 light-years
    Galactic period 2.25–2.50×108 a
    Velocity 2.17×105 m/s
    (orbit around the center of the Galaxy)

    2×104 m/s
    (relative to average velocity of other stars in stellar neighborhood)
    Physical characteristics
    Mean diameter 1.392×109 m [54]
    109 Earths
    Equatorial radius 6.955×108 m [56]
    Equatorial circumference 4.379×109 m [56]
    Flattening 9×10−6
    Surface area [[1 E+18 m²|6.088]]×1018 m² [56]
    11,900 Earths
    Volume [[1 E+27 m³|1.4122]]×1027 m³ [56]
    1,300,000 Earths
    Mass 1.9891 ×1030 kg[54]
    332,946 Earths
    Average density 1.409 ×103 kg/m³ [56]
    Equatorial surface gravity 274.0 m/s2 [54]
    27.94 g
    Escape velocity
    (from the surface)
    617.7 km/s [56]
    55 Earths
    Temperature
    of surface (effective)
    5,778 K [54]
    Temperature
    of corona
    ~5,000,000 K
    Temperature
    of core
    ~15,710,000 K [54]
    Luminosity (Lsol) 3.846×1026 W [54]
    ~3.75×1028 lm
    ~98 lm/W efficacy
    Mean Intensity (Isol) 2.009×107 W m-2 sr-1
    Rotation characteristics
    Obliquity 7.25° [54]
    (to the ecliptic)
    67.23°
    (to the galactic plane)
    Right ascension
    of North pole[57]
    286.13°
    19 h 4 min 30 s
    Declination
    of North pole
    +63.87°
    63°52' North
    Sidereal Rotation period
    (at 16° latitude)
    25.38 days [54]
    25 d 9 h 7 min 13 s[57]
    (at equator) 25.05 days [54]
    (at poles) 34.3 days [54]
    Rotation velocity
    (at equator)
    7.284 ×103 km/h
    Photospheric composition (by mass)
    Hydrogen 73.46 %
    Helium 24.85 %
    Oxygen 0.77 %
    Carbon 0.29 %
    Iron 0.16 %
    Sulfur 0.12 %
    Neon 0.12 %
    Nitrogen 0.09 %
    Silicon 0.07 %
    Magnesium 0.05 %

    The Sun (Latin: Sol) is the star at the center of the Solar System. The Earth and other matter (including other planets, asteroids, meteoroids, comets and dust) orbit the Sun, which by itself accounts for about 99.8% of the solar system's mass. Energy from the Sun, in the form of sunlight, supports almost all life on Earth via photosynthesis, and drives the Earth's climate and weather.

    The Sun is composed of hydrogen (about 74% of its mass, or 92% of its volume), helium (about 25% of mass, 7% of volume), and trace quantities of other elements. The Sun has a spectral class of G2V. G2 implies that it has a surface temperature of approximately 5,780 K, giving it a white color which, because of atmospheric scattering, appears yellow as seen from the surface of the Earth. This is a subtractive effect, as the preferential scattering of blue photons (causing the sky color) removes enough blue light to leave a residual reddishness that is perceived as yellow. (When low enough in the sky, the Sun appears orange or red, due to this scattering.)

    Its spectrum contains lines of ionized and neutral metals as well as very weak hydrogen lines. The V (Roman five) suffix indicates that the Sun, like most stars, is a main sequence star. This means that it generates its energy by nuclear fusion of hydrogen nuclei into helium and is in a state of hydrostatic equilibrium, neither contracting nor expanding over time. There are more than 100 million G2 class stars in our galaxy. Because of logarithmic size distribution, the Sun is actually brighter than 85% of the stars in the galaxy, most of which are red dwarfs.[1]

    The Sun orbits the center of the Milky Way galaxy at a distance of approximately 26,000 light-years from the galactic center, completing one revolution in about 225–250 million years. The orbital speed is 217 km/s, equivalent to one light-year every 1,400 years, and one AU every 8 days.[2]

    It is currently traveling through the Local Interstellar Cloud in the low-density Local Bubble zone of diffuse high-temperature gas, in the inner rim of the Orion Arm of the Milky Way Galaxy, between the larger Perseus and Sagittarius arms of the galaxy. Of the 50 nearest stellar systems within 17 light years from the Earth, the sun ranks 4th in absolute magnitude as a fourth magnitude star (M=4.83).

    Overview

    The Sun is a Population I, or third generation, star whose formation may have been triggered by shockwaves from one or more nearby supernovae.[3] This is suggested by a high abundance of heavy elements such as gold and uranium in the solar system. These elements could most plausibly have been produced by endergonic nuclear reactions during a supernova, or by transmutation via neutron absorption inside a massive second-generation star.

    Sunlight is Earth's primary source of energy. The solar constant is the amount of power that the Sun deposits per unit area that is directly exposed to sunlight. The solar constant is equal to approximately 1,370 watts per square meter of area at a distance of one AU from the Sun (that is, on or near Earth). Sunlight on the surface of Earth is attenuated by the Earth's atmosphere so that less power arrives at the surface—closer to 1,000 watts per directly exposed square meter in clear conditions when the Sun is near the zenith. This energy can be harnessed via a variety of natural and synthetic processes—photosynthesis by plants captures the energy of sunlight and converts it to chemical form (oxygen and reduced carbon compounds), while direct heating or electrical conversion by solar cells are used by solar power equipment to generate electricity or to do other useful work. The energy stored in petroleum and other fossil fuels was originally converted from sunlight by photosynthesis in the distant past.

    Ultraviolet light from the Sun has antiseptic properties and can be used to sanitize tools and water. It also causes sunburn, and has other medical effects such as the production of Vitamin D. Ultraviolet light is strongly attenuated by Earth's ozone layer, so that the amount of UV varies greatly with latitude. The angle that the Sun makes with Zenith at noon has been responsible for many biological adaptations, including variations in human skin color in different regions of the globe.[4]

    Observed from Earth, the Sun's path across the sky varies throughout the year. The shape described by the Sun's position, considered at the same time each day for a complete year, is called the analemma and resembles a figure 8 aligned along a north/south axis. While the most obvious variation in the Sun's apparent position through the year is a north/south swing over 47 degrees of angle (because of the 23.5-degree tilt of the Earth with respect to the Sun), there is an east/west component as well, caused by the acceleration of the Earth as it approaches its perihelion with the sun, and the reduction in the Earth's speed as it moves away to approach its aphelion. The north/south swing in apparent angle is the main source of seasons on Earth.

    The Sun is a magnetically active star. It supports a strong, changing magnetic field that varies year-to-year and reverses direction about every eleven years around solar maximum. The Sun's magnetic field gives rise to many effects that are collectively called solar activity, including sunspots on the surface of the Sun, solar flares, and variations in solar wind that carry material through the Solar System. Effects of solar activity on Earth include auroras at moderate to high latitudes, and the disruption of radio communications and electric power. Solar activity is thought to have played a large role in the formation and evolution of the Solar System. Solar activity changes the structure of Earth's outer atmosphere.

    Although it is the nearest star to Earth and has been intensively studied by scientists, many questions about the Sun remain unanswered, such as why its outer atmosphere has a temperature of over 1 million K while its visible surface (the photosphere) has a temperature of less than 6,000 K. Current topics of scientific inquiry include the Sun's regular cycle of sunspot activity, the physics and origin of flares and prominences, the magnetic interaction between the chromosphere and the corona, and the origin (propulsion source) of solar wind.

    Life cycle

    The Sun's current main sequence age, determined using computer models of stellar evolution and nucleocosmochronology, is thought to be about 4.57 billion years.[5]

    It is thought that about 4592.1 million years ago, the rapid collapse of a hydrogen molecular cloud led to the formation of a third generation T Tauri Population I star, the Sun, in a region of the Galactic Habitable Zone (GHZ). The nascent star assumed a nearly circular orbit about 26,000 light-years from the centre of the Milky Way Galaxy.[6]

    The Sun is about halfway through its main-sequence evolution, during which nuclear fusion reactions in its core fuse hydrogen into helium. Each second, more than 4 million tonnes of matter are converted into energy within the Sun's core, producing neutrinos and solar radiation; at this rate, the Sun will have so far converted around 100 Earth-masses of matter into energy. The Sun will spend a total of approximately 10 billion years as a main sequence star.

    The Sun does not have enough mass to explode as a supernova. Instead, in 4–5 billion years, it will enter a red giant phase, its outer layers expanding as the hydrogen fuel in the core is consumed and the core contracts and heats up. Helium fusion will begin when the core temperature reaches around 100 MK, and will produce carbon and oxygen, entering the asymptotic giant branch of a planetary nebula phase in about 7.8 billion years, during which instabilities in interior temperature lead the surface of the sun to shed mass. While it is likely that the expansion of the outer layers of the Sun will reach the current position of Earth's orbit, recent research suggests that mass lost from the Sun earlier in its red giant phase will cause the Earth's orbit to move further out, preventing it from being engulfed.[7] However, Earth's water will be boiled away and most of its atmosphere will escape into space. The increase in solar temperatures over this period is sufficient that by about 500-700 million years into the future, the surface of the Earth will become too hot for the survival of life as we know it.

    Life-cycle of the Sun
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    Life-cycle of the Sun


    Following the red giant phase, intense thermal pulsations will cause the Sun to throw off its outer layers, forming a planetary nebula. The only object that will remain after the outer layers are ejected is the extremely hot stellar core, which will slowly cool and fade as a white dwarf over many billions of years. This stellar evolution scenario is typical of low- to medium-mass stars.[7][8]

    Structure

    An illustration of the structure of the Sun
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    An illustration of the structure of the Sun

    The Sun is a yellow dwarf star. It comprises approximately 99% of the total mass of the solar system. The Sun is a near-perfect sphere, with an oblateness estimated at about 9 millionths,[9] which means that its polar diameter differs from its equatorial diameter by only 10 km (6 mi). As the Sun exists in a plasmatic state and is not solid, it undergoes differential rotation as it spins on its axis (i.e. it rotates faster at the equator than at the poles). The period of this actual rotation is approximately 25 days at the equator and 35 days at the poles. However, due to our constantly changing vantage point from the Earth as it orbits the Sun, the apparent rotation of the Sun at its equator is about 28 days. The centrifugal effect of this slow rotation is 18 million times weaker than the surface gravity at the Sun's equator. Also, the tidal effect from the planets does not significantly affect the shape of the Sun.

    The Sun does not have a definite boundary as rocky planets do; in its outer parts the density of its gases drops approximately exponentially with increasing distance from the center of the Sun. Nevertheless, the Sun has a well-defined interior structure, described below. The Sun's radius is measured from its center to the edge of the photosphere. This is simply the layer above which the gases are too cool or too thin to radiate a significant amount of light; the photosphere is the surface most readily visible to the naked eye. The solar core comprises 10 percent of its total volume, but 40 percent of its total mass.[10]

    The solar interior is not directly observable, and the Sun itself is opaque to electromagnetic radiation. However, just as seismology uses waves generated by earthquakes to reveal the interior structure of the Earth, the discipline of helioseismology makes use of pressure waves (infrasound) traversing the Sun's interior to measure and visualize the Sun's inner structure. Computer modeling of the Sun is also used as a theoretical tool to investigate its deeper layers.

    Core

    Cross-section of a solar-type star. (NASA)
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    Cross-section of a solar-type star. (NASA)

    The core of the Sun is considered to extend from the center to about 0.2 solar radii. It has a density of up to 150,000 kg/m³ (150 times the density of water on Earth) and a temperature of close to 13,600,000 kelvins (by contrast, the surface of the Sun is close to 5,785 kelvins (1/2350th of the core). Recent analysis of SOHO mission data favors a faster rotation rate in the core than in the rest of the radiative zone.[11] Through most of the Sun's life, energy is produced by nuclear fusion through a series of steps called the p–p (proton–proton) chain; this process converts hydrogen into helium. The core is the only location in the Sun that produces an appreciable amount of heat via fusion: the rest of the star is heated by energy that is transferred outward from the core. All of the energy produced by fusion in the core must travel through many successive layers to the solar photosphere before it escapes into space as sunlight or kinetic energy of particles.

    About 3.4×1038 protons (hydrogen nuclei) are converted into helium nuclei every second (out of ~8.9×1056 total amount of free protons in the Sun), releasing energy at the matter–energy conversion rate of 4.26 million tonnes per second, 383 yottawatts (3.83×1026 W) or 9.15×1010 megatons of TNT per second. This actually corresponds to a surprisingly low rate of energy production in the Sun's core—about 0.3 µW/cm³ (microwatts per cubic cm), or about 6 µW/kg of matter. For comparison, a candela of light (roughly one candle) produces heat at the rate 1 W/cm³, and the human body at approximately the rate 1.2 W/kg—millions of times more heat production. The use of plasma with similar parameters for energy production on Earth would be completely impractical—even a modest 1 GW fusion power plant would require about 170 billion tonnes of plasma occupying almost one cubic mile. Thus, terrestrial fusion reactors utilize far higher plasma temperatures than those in Sun's interior.

    The rate of nuclear fusion depends strongly on density and temperature, so the fusion rate in the core is in a self-correcting equilibrium: a slightly higher rate of fusion would cause the core to heat up more and expand slightly against the weight of the outer layers, reducing the fusion rate and correcting the perturbation; and a slightly lower rate would cause the core to cool and shrink slightly, increasing the fusion rate and again reverting it to its present level.

    The high-energy photons (cosmic, gamma and X-rays) released in fusion reactions are absorbed in only few millimetres of solar plasma and then re-emitted again in random direction (and at slightly lower energy)—so it takes a long time for radiation to reach the Sun's surface. Estimates of the "photon travel time" range from as much as 50 million years[12] to as little as 17,000 years.[13] After a final trip through the convective outer layer to the transparent "surface" of the photosphere, the photons escape as visible light. Each gamma ray in the Sun's core is converted into several million visible light photons before escaping into space. Neutrinos are also released by the fusion reactions in the core, but unlike photons they rarely interact with matter, so almost all are able to escape the Sun immediately. For many years measurements of the number of neutrinos produced in the Sun were lower than theories predicted by a factor of 3. This discrepancy was recently resolved through the discovery of the effects of neutrino oscillation: the sun in fact emits the number of neutrinos predicted by the theory, but neutrino detectors were missing 2/3 of them because the neutrinos had changed flavor.

    Radiation zone

    From about 0.2 to about 0.7 solar radii, solar material is hot and dense enough that thermal radiation is sufficient to transfer the intense heat of the core outward. In this zone there is no thermal convection; while the material grows cooler as altitude increases, this temperature gradient is less than the value of adiabatic lapse rate and hence cannot drive convection. Heat is transferred by radiationions of hydrogen and helium emit photons, which travel a brief distance before being reabsorbed by other ions. In this way energy makes its way very slowly (see above) outward.

    Convection zone

    Structure of the Sun
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    Structure of the Sun

    In the Sun's outer layer (down to approximately 70% of the solar radius), the solar plasma is not dense enough or hot enough to transfer the heat energy of the interior outward via radiation. As a result, thermal convection occurs as thermal columns carry hot material to the surface (photosphere) of the Sun. Once the material cools off at the surface, it plunges back downward to the base of the convection zone, to receive more heat from the top of the radiant zone. Convective overshoot is thought to occur at the base of the convection zone, carrying turbulent downflows into the outer layers of the radiant zone.

    The thermal columns in the convection zone form an imprint on the surface of the Sun, in the form of the solar granulation and supergranulation. The turbulent convection of this outer part of the solar interior gives rise to a "small-scale" dynamo that produces magnetic north and south poles all over the surface of the Sun.

    Photosphere

    The visible surface of the Sun, the photosphere, is the layer below which the Sun becomes opaque to visible light. Above the photosphere visible sunlight is free to propagate into space, and its energy escapes the Sun entirely. The change in opacity is due to the decreasing amount of H- ions, which absorb visible light easily. Conversely, the visible light we see is produced as electrons react with hydrogen atoms to produce H- ions.[14][15] The photosphere is actually tens to hundreds of kilometers thick, being slightly less opaque than air on Earth. Because the upper part of the photosphere is cooler than the lower part, an image of the Sun appears brighter in the center than on the edge or limb of the solar disk, in a phenomenon known as limb darkening. Sunlight has approximately a black-body spectrum that indicates its temperature is about 6,000 K, interspersed with atomic absorption lines from the tenuous layers above the photosphere. The photosphere has a particle density of about 1023 m−3 (this is about 1% of the particle density of Earth's atmosphere at sea level).

    During early studies of the optical spectrum of the photosphere, some absorption lines were found that did not correspond to any chemical elements then known on Earth. In 1868, Norman Lockyer hypothesized that these absorption lines were because of a new element which he dubbed "helium", after the Greek Sun god Helios. It was not until 25 years later that helium was isolated on Earth.[16]

    Atmosphere

    During a total solar eclipse, the solar corona can be seen with the naked eye.
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    During a total solar eclipse, the solar corona can be seen with the naked eye.

    The parts of the Sun above the photosphere are referred to collectively as the solar atmosphere. They can be viewed with telescopes operating across the electromagnetic spectrum, from radio through visible light to gamma rays, and comprise five principal zones: the temperature minimum, the chromosphere, the transition region, the corona, and the heliosphere. The heliosphere, which may be considered the tenuous outer atmosphere of the Sun, extends outward past the orbit of Pluto to the heliopause, where it forms a sharp shock front boundary with the interstellar medium. The chromosphere, transition region, and corona are much hotter than the surface of the Sun; the reason why is not yet known.

    The coolest layer of the Sun is a temperature minimum region about 500 km above the photosphere, with a temperature of about 4,000 K. This part of the Sun is cool enough to support simple molecules such as carbon monoxide and water, which can be detected by their absorption spectra.

    Above the temperature minimum layer is a thin layer about 2,000 km thick, dominated by a spectrum of emission and absorption lines. It is called the chromosphere from the Greek root chroma, meaning color, because the chromosphere is visible as a colored flash at the beginning and end of total eclipses of the Sun. The temperature in the chromosphere increases gradually with altitude, ranging up to around 100,000 K near the top.

    Taken by Hinode's Solar Optical Telescope on January 12, 2007, this image of the Sun reveals the filamentary nature of the plasma connecting regions of different magnetic polarity.
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    Taken by Hinode's Solar Optical Telescope on January 12, 2007, this image of the Sun reveals the filamentary nature of the plasma connecting regions of different magnetic polarity.

    Above the chromosph