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{{Short description|Star at the center of the Solar System}}
{{Sprotected2}}
:''For other uses, see ].'' {{Redirects|The Sun|other uses|Sun (disambiguation)|and|The Sun (disambiguation)}}
{{Featured article}}
{{Pp-semi-indef}}
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{{Use American English|date=August 2019}}
{{Use dmy dates|date=August 2019}}
{{CS1 config|mode=cs1}}
{{Infobox
| title = Sun
| image = ]
| caption = The Sun, viewed through a clear ]<!--no need to add more, for consistency with other planets and minor planets infobox-->
| labelstyle = background: inherit;
| label1 = Names
| data1 = Sun, ],<ref name=OED /> ], ]<ref name=Lexico />
| label2 = Adjectives
| data2 = Solar<ref name=OED2 />
| label3 = ]
| data3 = ]
| header4 = Observation data
| label5 = Mean distance from Earth
| data5 = {{val|1|ul=AU}}<br />149,600,000 km<br />8&nbsp;min 19&nbsp;s, ]<ref name="Pitjeva2009">{{Cite journal |last1=Pitjeva |first1=E. V. |last2=Standish |first2=E. M. |year=2009 |title=Proposals for the masses of the three largest asteroids, the Moon–Earth mass ratio and the Astronomical Unit |url=https://zenodo.org/record/1000691 |url-status=live |journal=] |volume=103 |issue=4 |pages=365–372 |bibcode=2009CeMDA.103..365P |doi=10.1007/s10569-009-9203-8 |issn=1572-9478 |s2cid=121374703 |archive-url=https://web.archive.org/web/20190709062657/https://zenodo.org/record/1000691 |archive-date=9 July 2019 |access-date=13 July 2019}}</ref>
| label6 = {{longitem|]}}
| data6 = −26.74 (''V'')<ref name="nssdc">{{Cite web |last=Williams |first=D. R. |date=1 July 2013 |title=Sun Fact Sheet |url=http://nssdc.gsfc.nasa.gov/planetary/factsheet/sunfact.html |url-status=live |archive-url=https://web.archive.org/web/20100715200549/http://nssdc.gsfc.nasa.gov/planetary/factsheet/sunfact.html |archive-date=15 July 2010 |access-date=12 August 2013 |publisher=]}}</ref>
| label7 = {{longitem|]}}
| data7 = 4.83<ref name="nssdc" />
| label8 = {{longitem|]}}
| data8 = G2V<ref>{{Cite book |last=Zombeck |first=Martin V. |url=http://ads.harvard.edu/books/hsaa/ |title=Handbook of Space Astronomy and Astrophysics 2nd edition |year=1990 |publisher=] |access-date=13 January 2016 |archive-url=https://web.archive.org/web/20210203012304/http://ads.harvard.edu/books/hsaa/ |archive-date=3 February 2021 |url-status=live}}</ref>
| label9 = ]
| data9 = ''Z'' = 0.0122<ref>{{Cite journal |last1=Asplund |first1=M. |last2=Grevesse |first2=N. |last3=Sauval |first3=A. J. |year=2006 |title=The new solar abundances – Part I: the observations |journal=Communications in Asteroseismology |volume=147 |pages=76–79 |bibcode=2006CoAst.147...76A |doi=10.1553/cia147s76 |s2cid=123824232 |doi-access=free| issn = 1021-2043}}</ref>
| label10 = ]
| data10 = 0.527–0.545°<ref>{{Cite web |title=Eclipse 99: Frequently Asked Questions |url=http://education.gsfc.nasa.gov/eclipse/pages/faq.html |url-status=dead |archive-url=https://web.archive.org/web/20100527142627/http://education.gsfc.nasa.gov/eclipse/pages/faq.html |archive-date=27 May 2010 |access-date=24 October 2010 |publisher=NASA}}</ref>
| header11 = Orbital characteristics
| label12 = {{longitem|Mean distance from ] core}}
| data12 = 24,000 to 28,000 ]s<ref name="francis14">{{cite journal |last1=Francis |first1=Charles |last2=Anderson |first2=Erik |date=June 2014 |title=Two estimates of the distance to the Galactic Centre |journal=] |volume=441 |issue=2 |pages=1105–1114 |arxiv=1309.2629 |bibcode=2014MNRAS.441.1105F |doi=10.1093/mnras/stu631 |doi-access=free |s2cid=119235554}}</ref>
| label13 = ]
| data13 = 225–250 million ]
| label14 = ]
| data14 = {{indented plainlist|
<!-- -->*251 km/s<br />orbit ]
<!-- -->*20 km/s<br />to stellar neighborhood
<!-- -->*370 km/s<br />to ]<ref>{{Cite journal | display-authors=5 | last1=Hinshaw | first1=G. | last2=Weiland | first2=J. L. | last3=Hill | first3=R. S. | last4=Odegard | first4=N. | last5=Larson | first5=D. | last6=Bennett | first6=C. L. | last7=Dunkley | first7=J. | last8=Gold | first8=B. | last9=Greason | first9=M. R. | last10=Jarosik | first10=N. | last11=Komatsu | first11=E. | last12=Nolta | first12=M. R. | last13=Page | first13=L. | last14=Spergel | first14=D. N. | last15=Wollack | first15=E. | last16=Halpern | first16=M. | last17=Kogut | first17=A. | last18=Limon | first18=M. | last19=Meyer | first19=S. S. | last20=Tucker | first20=G. S. | last21=Wright | first21=E. L. |year=2009 |title=Five-year Wilkinson Microwave Anisotropy Probe observations: data processing, sky maps, and basic results |journal=] |volume=180 |issue=2 |pages=225–245 |arxiv=0803.0732 |bibcode=2009ApJS..180..225H |doi=10.1088/0067-0049/180/2/225 |s2cid=3629998}}</ref>
}}
| label15 = ]
| data15 = {{unbulleted list|
|7.25° (])<ref name=nssdc />
|67.23° (])
}}
| label16 = {{longitem|] North pole}}
| data16 = 286.13° (286° 7′ 48″)<ref name="nssdc" />
| label17 = {{longitem|] of North pole}}
| data17 = +63.87° (63° 52′ 12"N)<ref name="nssdc" />
| label18 = {{longitem|Sidereal ]}}
| data18 = {{unbulleted list
|25.05 days (equator)
|34.4 days (poles)<ref name=nssdc /><!-- derived from T = ( 14.37 − 2.33 sin^2 L − 1.56 sin^4 L ) °/day, L = 90° -->
}}
| label19 = {{longitem|Equatorial rotation velocity}}
| data19 = {{val|1.997|u=km/s}}<ref name="sse">{{Cite web |title=Solar System Exploration: Planets: Sun: Facts & Figures |url=http://solarsystem.nasa.gov/planets/profile.cfm?Object=Sun&Display=Facts&System=Metric |url-status=dead |archive-url=https://web.archive.org/web/20080102034758/http://solarsystem.nasa.gov/planets/profile.cfm?Object=Sun&Display=Facts&System=Metric |archive-date=2 January 2008 |publisher=NASA}}</ref><!-- Derived from NASA source: equatorial circumference of 4,379,000 kilometers divided by sidereal rotation period of 609.12 hours; maybe this kind of basic calculation could be done in some generic template code? -->
| header20 = Physical characteristics
| label21 = {{longitem|Equatorial ]}}
| data21 = {{val|6.957|e=8|u=m}}<ref name="IAU2015resB3">{{Cite journal |last1=Prša |first1=Andrej |last2=Harmanec |first2=Petr |last3=Torres |first3=Guillermo |last4=Mamajek |first4=Eric |last5=Asplund |first5=Martin |last6=Capitaine |first6=Nicole |last7=Christensen-Dalsgaard |first7=Jørgen |last8=Depagne |first8=Éric |last9=Haberreiter |first9=Margit |last10=Hekker |first10=Saskia |last11=Hilton |first11=James |last12=Kopp |first12=Greg |last13=Kostov |first13=Veselin |last14=Kurtz |first14=Donald W. |last15=Laskar |first15=Jacques |display-authors=3 |date=2016-08-01 |title=NOMINAL VALUES FOR SELECTED SOLAR AND PLANETARY QUANTITIES: IAU 2015 RESOLUTION B3 * † |journal=The Astronomical Journal |volume=152 |issue=2 |pages=41 |doi=10.3847/0004-6256/152/2/41 |issn=0004-6256 |arxiv=1510.07674 |last16=Laskar |first16=J. |last17=Mason |first17=B. D. |last18=Milone |first18=E. F. |last19=Montgomery |first19=M. M. |last20=Richards |first20=M. T. |last21=Schou |first21=J. |last22=Stewart |first22=S. G.|doi-access=free }}</ref><br />{{val|109|u=× ]}}<ref name=sse />
| label23 = ]
| data23 = 0.00005<ref name="nssdc" />
| label24 = ]
| data24 = {{val|6.09|e=12|u=km2}}<br />{{nowrap|{{val|fmt=commas|12000}}}} × Earth<ref name=sse />
| label25 = ]
| data25 = {{unbulleted list
|{{val|1.412|e=18|u=km3}}
|{{val|fmt=commas|1300000}} × Earth
}}
| label26 = ]
| data26 = {{unbulleted list
|{{val|1.9885|e=30|u=kg}}<ref name="nssdc" />
|{{val|fmt=commas|332950|u=]}}<ref name=nssdc /><!-- NASA Sun Fact Sheet states 333,000, a figure coherent with data already present in en.wiki -->
}}
| label27 = Average ]
| data27 = {{val|1.408|u=g/cm3}}<br />{{val|0.255}} × Earth<ref name=nssdc /><ref name=sse />
| label28 = Age
| data28 = 4.6 billion years<ref name="Bonanno">{{Cite journal |last1=Bonanno |first1=A. |last2=Schlattl |first2=H. |last3=Paternò |first3=L. |year=2002 |title=The age of the Sun and the relativistic corrections in the EOS |journal=] |volume=390 |issue=3 |pages=1115–1118 |arxiv=astro-ph/0204331 |bibcode=2002A&A...390.1115B |doi=10.1051/0004-6361:20020749 |s2cid=119436299}}</ref><ref>{{Cite journal |last1=Connelly |first1=J. N. |last2=Bizzarro |first2=M. |last3=Krot |first3=A. N. |last4=Nordlund |first4=Å. |last5=Wielandt |first5=D. |last6=Ivanova |first6=M. A. |date=2 November 2012 |title=The Absolute Chronology and Thermal Processing of Solids in the Solar Protoplanetary Disk |journal=Science |volume=338 |issue=6107 |pages=651–655 |bibcode=2012Sci...338..651C |doi=10.1126/science.1226919 |pmid=23118187 |s2cid=21965292}}{{Registration required}}</ref>
| label29 = {{longitem|Equatorial ]}}
| data29 = {{val|274|u=m/s2}}<ref name=nssdc /><br />{{cvt|274|m/s2|g0|disp=out|lk=out}}<ref name=sse />
| label30 = {{longitem|]}}
| data30 = ≈{{val|0.070}}<ref name=nssdc />
| label31 = {{longitem|Surface ]}}
| data31 = {{val|617.7|u=km/s}}<br />55 × Earth<ref name=sse />
| label32 = Temperature
| data32 = {{unbulleted list|
|15,700,000 ] (center)<ref name=nssdc />
|5,772 K (])<ref name="IAU2015resB3"/>
|5,000,000 K (])
}}
| label33 = ]
| data33 = {{unbulleted list|
|{{val|3.828|e=26|ul=W}}<ref name=nssdc />
|{{val|3.75|e=28|u=]}}
|{{val|98|u=lm/W}} ]
}}
| label34 = ] (B-V)
| data34 = 0.656<ref>{{cite journal | first=David F. | last=Gray | title=The Inferred Color Index of the Sun | journal=Publications of the Astronomical Society of the Pacific | volume=104 | issue=681 | pages=1035–1038 | date=November 1992 | doi=10.1086/133086 | bibcode=1992PASP..104.1035G }}</ref>
| label35 = Mean ]
| data35 = {{val|2.009|e=7|u=W·m<sup>−2</sup>·sr<sup>−1</sup>}}
| label37 = {{longitem|] composition by mass}}
| data37 = {{unbulleted list|
| 73.46% ]
| 24.85% ]
| 0.77% ]
| 0.29% ]
| 0.16% ]
| 0.12% ]
| 0.09% ]
| 0.07% ]
| 0.05% ]
| 0.04% ]<ref>{{Cite web |title=The Sun's Vital Statistics |url=http://solar-center.stanford.edu/vitalstats.html |url-status=live |archive-url=https://www.webcitation.org/6BOkQXma3?url=http://solar-center.stanford.edu/vitalstats.html |archive-date=14 October 2012 |access-date=29 July 2008 |publisher=Stanford Solar Center}} Citing {{cite book |last=Eddy |first=J. |date=1979 |title=A New Sun: The Solar Results From Skylab |url=https://history.nasa.gov/SP-402/contents.htm |page=37 |publisher=NASA |id=NASA SP-402 |access-date=12 July 2017 |archive-date=30 July 2021 |archive-url=https://web.archive.org/web/20210730024856/https://history.nasa.gov/SP-402/contents.htm |url-status=live }}</ref>
}}
}}


The '''Sun''' is the ] at the center of the ]. It is a massive, nearly perfect ] of hot ], heated to ] by ] reactions in its core, radiating the energy from its ] mainly as ] and ] with 10% at ] energies. It is by far the most important source of energy for ] on ]. The Sun has been an ] in many cultures. It has been a central subject for astronomical research since ].
{| border="2" cellpadding="4" cellspacing="0" style="margin: 0 0 1em 1em; border: 1px #aaa solid; border-collapse: collapse;" align="right" width=280px
|+
|+ style="font-size:larger;" | '''The Sun''' ]
|+
|-
| colspan="2" align="center" | ]
|-
! bgcolor="#ffffc0" colspan="2" align="center" | '''Observation data'''
|-
! align="left" | Mean distance from<br>]
| ]{{e|6}}&nbsp;]<br>(92.95{{e|6}} ]) <br>(8.31 minutes at the ])
|-
! align="left" | ] (''V'')
| &minus;26.8<sup>m</sup>
|-
! align="left" | ]
| 4.8<sup>m</sup>
|-
! align="left" | ]
| G2V
|-
! bgcolor="#ffffc0" colspan="2" align="center" | ''']al characteristics'''
|-
! align="left" | Mean distance from<br>] core
| ~2.5{{e|17}}&nbsp;km <br>(26,000-28,000 ]s)
|-
! align="left" | ] period
| 2.25-2.50{{e|8}} ]
|-
! align="left" | Velocity
| 217&nbsp;km/] orbit around the center of the Galaxy, 20&nbsp;km/s relative to average velocity of other stars in stellar neighborhood
|-
! bgcolor="#ffffc0" colspan="2" align="center" | '''Physical characteristics'''
|-
! align="left" | Mean diameter
| ]{{e|6}}&nbsp;km<br>(109 Earth diameters)
|-
! align="left" | Circumference
| ]{{e|6}}&nbsp;km<br>(342 Earth diameters)
|-
! align="left" | ]
| 9{{e|&minus;6}}
|-
! align="left" | Surface area
| ]{{e|12}}&nbsp;]<br>(11,900 Earths)
|-
! align="left" | Volume
| ]{{e|18}}&nbsp;]<br>(1,300,000 Earths)
|-
! align="left" | Mass
| 1.988&thinsp;435{{e|30}}&nbsp;]<br>
(332,946 Earths)
|-
! align="left" | Density
| 1.408&nbsp;g/cm³
|-
! align="left" | Surface ]
| 273.95&nbsp;m s<sup>-2</sup><br>
(27.9 ])
|-
! align="left" | ]<br> from the surface
| 617.54&nbsp;km/s
(55 Earths)
|-
! align="left" | Surface temperature
| 5785&nbsp;]
|-
! align="left" | Temperature of ]
| 5&nbsp;]K
|-
! align="left" | Core temperature
| ~13.6&nbsp;MK
|-
! align="left" | ] (''L<sub>sol</sub>'')
| 3.827{{e|26}}&nbsp;]<br/>~3.75{{e|28}}&nbsp;]<br/>(~98&nbsp;lm/W ])
|-
! align="left" | Mean ] (''I<sub>sol</sub>'')
| 2.009{{e|7}}&nbsp;W m<sup>-2</sup> sr<sup>-1</sup>
|-
! bgcolor="#ffffc0" colspan="2" align="center" | '''] characteristics'''
|-
! align="left" | ]
| 7.25] <br>(to the ]) <br>67.23° <br>(to the ])
|-
! align="left" | ]<br>of North pole<ref name="iau-iag">{{cite web
|url=http://www.hnsky.org/iau-iag.htm
|title=Report Of The IAU/IAG Working Group On Cartographic Coordinates And Rotational Elements Of The Planets And Satellites: 2000
|accessdate=2006-03-22
|first=P. K.
|last=Seidelmann
|coauthors=V. K. Abalakin; M. Bursa; M. E. Davies; C. de Bergh; J. H. Lieske; J. Oberst; J. L. Simon; E. M. Standish; P. Stooke; P. C. Thomas
|year=2000}}</ref>
| 286.13° <br>(19 h 4 min 30 s)
|-
! align="left" | ]<br>of North pole
| +63.87°<br>(63°52' North)
|-
! align="left" | ]<br>at equator
| 25.3800 days <br>(25 d 9 h 7 min 13 s)<ref name="iau-iag"/>
|-
! align="left" | Rotation velocity<br>at equator
| 7174&nbsp;km/h
|-
! bgcolor="#ffffc0" colspan="2" align="center" | '''] composition (by mass)'''
|-
! align="left" | ]
| 73.46 %
|-
! align="left" | ]
| 24.85 %
|-
! align="left" | ]
| 0.77 %
|-
! align="left" | ]
| 0.29 %
|-
! align="left" | ]
| 0.16 %
|-
! align="left" | ]
| 0.12 %
|-
! align="left" | ]
| 0.09 %
|-
! align="left" | ]
| 0.07 %
|-
! align="left" | ]
| 0.05 %
|-
! align="left" | ]
| 0.04 %
|}
The '''Sun''' is the ] of our ]. The Earth and other matter (including other ]s, ]s, ]s, ]s and ]) ] the Sun, which by itself accounts for more than 99% of the solar system's ]. ] from the Sun—in the form of ] from ]—supports almost all life on Earth via ], and drives the Earth's ] and weather.


The Sun orbits the ] at a distance of 24,000 to 28,000 ]s. From Earth, it is {{val|1|u=]}} ({{val|1.496|e=8|u=km}}) or about 8 ]s away. ] is about {{val|1391400|u=km|fmt=commas}} ({{val|864600|u=mi|fmt=commas}}), 109 times that of Earth. ] is about 330,000 times that of Earth, making up about 99.86% of the total mass of the Solar System. Roughly three-quarters of the Sun's ] consists of ] (~73%); the rest is mostly ] (~25%), with much smaller quantities of heavier elements, including ], ], ], and ].
The Sun is sometimes referred to by its ] name '']'' or by its ] name '']''. Its ] and ] is a ]: ]. Some ancient peoples of the world considered it a ] before the acceptance of ].


The Sun is a ] (G2V), informally called a yellow dwarf, though its light is actually white. It formed approximately 4.6&nbsp;billion<ref group=lower-alpha name=short>All numbers in this article are ]. One billion is 10<sup>9</sup>, or 1,000,000,000.</ref> years ago from the ] of matter within a region of a large ]. Most of this matter gathered in the center, whereas the rest flattened into an orbiting disk that ]. The central mass became so hot and dense that it eventually initiated ] in its ]. Every second, the Sun's core fuses about 600&nbsp;billion ] (kg) of hydrogen into helium and converts 4&nbsp;billion kg of ].
==Overview==
] from the surface of Earth.]]
About 74% of the Sun's mass is ], 25% is ], and the rest is made up of trace quantities of heavier elements.
The Sun has a ] of G2V. "G2" means that it has a surface temperature of approximately 5,500&nbsp;K, giving it a ] color, which because of atmospheric ] appears yellow. Its spectrum contains ]s of ionized and neutral metals as well as very weak hydrogen lines. The "V" suffix indicates that the Sun, like most stars, is a ] star. This means that it generates its energy by ] of ] nuclei into ] and is in a state of ], 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 ].<ref> http://www.space.com/scienceastronomy/060130_mm_single_stars.html</ref>


About 4 to 7 billion years from now, when ] in the Sun's core diminishes to the point where the Sun is no longer in ], its core will undergo a marked increase in density and temperature which will cause its outer layers to expand, eventually transforming the Sun into a ]. This process will make the Sun large enough to render Earth uninhabitable approximately five billion years from the present. After the red giant phase, models suggest the Sun will shed its outer layers and become a dense type of cooling star (a ]), and no longer produce energy by fusion, but will still glow and give off heat from its previous fusion for perhaps trillions of years. After that, it is theorized to become a super dense ], giving off negligible energy.
The Sun orbits the center of the ] ] at a distance of approximately 25,000 to 28,000 ]s from the ], completing one revolution in about ]. The ] is 217&nbsp;km/s, equivalent to one light-year every 1,400 years, and one ] every 8 days.<ref name="Kerr">{{cite journal
|last=Kerr
|first=F. J.
|coauthors=Lynden-Bell D.
|year=1986
|url=http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1986MNRAS.221.1023K&amp;data_type=PDF_HIGH&amp;type=PRINTER&amp;filetype=.pdf
|title=Review of galactic constants
|journal=Monthly Notices of the Royal Astronomical Society
|volume=221
|pages=1023-1038}}</ref>


== Etymology ==
The Sun is a ] star, whose formation may have been triggered by shockwaves from a nearby ]. This is suggested by a high ] of ] such as ] and ] in the solar system; these elements could most plausibly have been produced by ] nuclear reactions during a supernova, or by ] via ] absorption inside a massive second-generation star.
The English word ''sun'' developed from ] {{lang|ang|sunne}}. Cognates appear in other ], including ] {{lang|fy|sinne}}, ] {{lang|nl|zon}}, ] {{lang|nds|Sünn}}, ] {{lang|de|Sonne}}, ] {{lang|bar|Sunna}}, ] {{lang|non|sunna}}, and ] {{lang|got|sunnō}}. All these words stem from ] {{lang|gem-x-proto|*sunnōn}}.<ref name="BARNHART776">{{Cite book |last=Barnhart |first=R. K. |title=The Barnhart Concise Dictionary of Etymology |year=1995 |publisher=] |isbn=978-0-06-270084-1 |page=776}}</ref><ref name="Orel">{{cite book|last=Orel|first=Vladimir|author-link=Vladimir Orel|year=2003|title=A Handbook of Germanic Etymology|page=|url=https://archive.org/details/Orel-AHandbookOfGermanicEtymology/mode/2up|via=]|publisher=Brill|place=Leiden|isbn=978-9-00-412875-0}}</ref> This is ultimately related to the word for ''sun'' in other branches of the ] family, though in most cases a ] stem with an ''l'' is found, rather than the ] stem in ''n'', as for example in ] {{lang|la|sōl}}, ] {{lang|grc|ἥλιος}} ({{transliteration|grc|hēlios}}), ] {{lang|cy|haul}} and ] {{lang|cs|slunce}}, as well as (with *l > ''r'') Sanskrit {{lang|sa|स्वर्}} ({{transliteration|sa|svár}}) and ] {{lang|fa|خور}} ({{transliteration|fa|xvar}}). Indeed, the ''l''-stem survived in Proto-Germanic as well, as {{lang|gem-x-proto|*sōwelan}}, which gave rise to Gothic {{lang|got|sauil}} (alongside {{lang|got|sunnō}}) and Old Norse prosaic {{lang|non|sól}} (alongside poetic {{lang|non|sunna}}), and through it the words for ''sun'' in the modern Scandinavian languages: ] and ] {{lang|sv|sol}}, ] {{lang|is|sól}}, etc.<ref name=Orel />


The principal adjectives for the Sun in English are ''sunny'' for sunlight and, in technical contexts, ''solar'' ({{IPAc-en|ˈ|s|oʊ|l|ər}}),<ref name="OED2">{{OED|solar}}</ref> from Latin {{lang|la|sol}}.<ref>{{cite dictionary |last1=Little |first1=William |dictionary=Oxford Universal Dictionary on Historical Principles |last2=Fowler |first2=H. W. |last3=Coulson |first3=J. |year=1955 |edition=3rd |title=Sol |asin=B000QS3QVQ |url=https://archive.org/details/oxforduniversald07litt |url-access=registration}}</ref> From the Greek {{transliteration|grc|helios}} comes the rare adjective ''heliac'' ({{IPAc-en|ˈ|h|iː|l|i|æ|k}}).<ref>{{OED|heliac}}</ref> In English, the Greek and Latin words occur in poetry as personifications of the Sun, ] ({{IPAc-en|ˈ|h|iː|l|i|ə|s}}) and ] ({{IPAc-en|'|s|ɒ|l}}),<ref name="Lexico">{{Cite dictionary |title=Helios |dictionary=] UK English Dictionary |publisher=] |url=http://www.lexico.com/definition/Helios |archive-url=https://web.archive.org/web/20200327234645/https://www.lexico.com/definition/helios |archive-date=27 March 2020 |url-status=dead}}</ref><ref name="OED">{{OED|Sol}}</ref> while in science fiction ''Sol'' may be used to distinguish the Sun from other stars. The term '']'' with a lowercase ''s'' is used by planetary astronomers for the duration of a ] on another planet such as ].<ref>{{Cite web |date=15 November 2006 |title=Opportunity's View, Sol 959 (Vertical) |url=http://www.nasa.gov/mission_pages/mer/images/pia01892.html |url-status=live |archive-url=https://web.archive.org/web/20121022155351/http://www.nasa.gov/mission_pages/mer/images/pia01892.html |archive-date=22 October 2012 |access-date=1 August 2007 |publisher=]}}</ref>
Sunlight is the main source of energy near the surface of Earth. The ] 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&nbsp;]s per square meter of area at a distance of one ] from the Sun (that is, on or near Earth). Sunlight on the surface of Earth is ] by the Earth's atmosphere so that less power arrives at the surface&mdash;closer to 1,000&nbsp;watts per directly exposed square meter in clear conditions when the Sun is near the ]. This energy can be harnessed via a variety of natural and synthetic processes&mdash;] 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 ] are used by ] equipment to generate ] or to do other useful work. The energy stored in ] and other ] was originally converted from sunlight by photosynthesis in the distant past.


The ] for the Sun is a circle with a center dot, ].<ref>{{cite book |last1=Allen |first1=Clabon W. |author-link1=Clabon Allen |last2=Cox |first2=Arthur N. |editor-last=Cox |editor-first=Arthur N. |year=2000 |title=Allen's Astrophysical Quantities |page=2 |publisher=Springer |edition=4th |isbn=978-0-38-798746-0 |url=https://books.google.com/books?id=w8PK2XFLLH8C|via=]}}</ref> It is used for such units as ''M''<sub>☉</sub> (]), ''R''<sub>☉</sub> (]) and ''L''<sub>☉</sub> (]).<ref>{{Cite dictionary |title=solar mass |url=https://www.oxfordreference.com/display/10.1093/oi/authority.20110803100516843 |access-date=2024-05-26 |dictionary=Oxford Reference }}</ref><ref>{{Cite book |last1=Weissman |first1=Paul |url=https://books.google.com/books?id=4gmSOrXIQUEC&dq=%22solar+radius%22&pg=PA349 |title=Encyclopedia of the Solar System |last2=McFadden |first2=Lucy-Ann |last3=Johnson |first3=Torrence |date=1998-09-18 |publisher=Academic Press |isbn=978-0-08-057313-7 |pages=349, 820}}</ref>
Sunlight has several interesting biological properties. ] light from the Sun has ] properties and can be used to sterilize tools. It also causes ], and has other medical effects such as the production of ]. Ultraviolet light is strongly attenuated by Earth's atmosphere, so that the amount of UV varies greatly with ] because of the longer passage of sunlight through the atmosphere at high latitudes. This variation is responsible for many biological adaptations, including variations in human ] in different regions of the globe.
The scientific study of the Sun is called ''heliology''.<ref>{{cite dictionary |url=https://www.collinsdictionary.com/dictionary/english/heliology |title=heliology |publisher=Collins |dictionary=Collins Dictionary |access-date=24 November 2024 }}</ref>


== General characteristics ==
Observed from Earth, the path of the Sun 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 ] 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. The North/South swing in apparent angle is the main source of ] on Earth.
] the ] and some larger stars. The Sun is 1.4 million kilometers (4.643 ]s) wide, about 109 times ] Earth, or four times the ], and contains 99.86% of all Solar System ].]]


The Sun is a ] that makes up about 99.86% of the mass of the Solar System.<ref name="Woolfson00">{{Cite journal |last=Woolfson |first=M. |date=2000 |title=The origin and evolution of the solar system |url=http://inis.jinr.ru/sl/vol1/_djvu/P_Physics/Woolfson%20M.M.%20Origin%20and%20evolution%20of%20the%20solar%20system%20(IOP)(425s).pdf |url-status=live |journal=] |volume=41 |issue=1 |page=12 |bibcode=2000A&G....41a..12W |doi=10.1046/j.1468-4004.2000.00012.x |archive-url=https://web.archive.org/web/20200711133403/http://inis.jinr.ru/sl/vol1/_djvu/P_Physics/Woolfson%20M.M.%20Origin%20and%20evolution%20of%20the%20solar%20system%20(IOP)(425s).pdf |archive-date=11 July 2020 |access-date=12 April 2020 |doi-access=free}}</ref><!-- There are several estimations on the mass of the Solar System; for further information please have a look at the talk page. --> It has an ] of +4.83, estimated to be brighter than about 85% of the stars in the ], most of which are ]s.<ref>{{Cite news |last=Than |first=K. |date=2006 |title=Astronomers Had it Wrong: Most Stars are Single |publisher=Space.com |url=http://www.space.com/scienceastronomy/060130_mm_single_stars.html |url-status=live |access-date=1 August 2007 |archive-url=https://web.archive.org/web/20101221093125/http://www.space.com/scienceastronomy/060130_mm_single_stars.html |archive-date=21 December 2010}}</ref><ref>{{Cite journal |last=Lada |first=C. J. |year=2006 |title=Stellar multiplicity and the initial mass function: Most stars are single |journal=] |volume=640 |issue=1 |pages=L63–L66 |arxiv=astro-ph/0601375 |bibcode=2006ApJ...640L..63L |doi=10.1086/503158 |s2cid=8400400}}</ref> It is more massive than 95% of the stars within {{cvt|7|pc|ly}}.<ref>{{cite journal |last1=Robles |first1=José A. |last2=Lineweaver |first2=Charles H. |last3=Grether |first3=Daniel |last4=Flynn |first4=Chris |last5=Egan |first5=Chas A. |last6=Pracy |first6=Michael B. |last7=Holmberg |first7=Johan |last8=Gardner |first8=Esko |title=A Comprehensive Comparison of the Sun to Other Stars: Searching for Self-Selection Effects |journal=The Astrophysical Journal |date=September 2008 |volume=684 |issue=1 |pages=691–706 |doi=10.1086/589985 |arxiv=0805.2962 |bibcode=2008ApJ...684..691R |hdl=1885/34434 |url=https://iopscience.iop.org/article/10.1086/589985/fulltext/73840.text.html |access-date=24 May 2024}}</ref>
The Sun is a magnetically active star; it supports a strong, changing ] that varies year-to-year and reverses direction about every eleven years. The Sun's magnetic field gives rise to many effects that are collectively called ], including ]s on the surface of the Sun, ], and variations in the ] that carry material through the solar system. The effects of solar activity on Earth include ]s at moderate to high latitudes, and the disruption of radio communications and ]. Solar activity is thought to have played a large role in the ] and evolution of the ], and strongly affects the structure of Earth's ].
The Sun is a ], or heavy-element-rich,{{efn|name=heavy elements}} star.<ref name="zeilik">{{Cite book |last1=Zeilik |first1=M. A. |title=Introductory Astronomy & Astrophysics |last2=Gregory |first2=S. A. |year=1998 |publisher=Saunders College Publishing |isbn=978-0-03-006228-5 |edition=4th |page=322}}</ref> Its formation approximately 4.6&nbsp;billion years ago may have been triggered by shockwaves from one or more nearby ]e.<ref name="Connelly2012">{{Cite journal |last1=Connelly |first1=James N. |last2=Bizzarro |first2=Martin |last3=Krot |first3=Alexander N. |last4=Nordlund |first4=Åke |last5=Wielandt |first5=Daniel |last6=Ivanova |first6=Marina A. |date=2 November 2012 |title=The Absolute Chronology and Thermal Processing of Solids in the Solar Protoplanetary Disk |journal=] |volume=338 |issue=6107 |pages=651–655 |bibcode=2012Sci...338..651C |doi=10.1126/science.1226919 |pmid=23118187 |s2cid=21965292}}</ref><ref name="Falk">{{Cite journal |last1=Falk |first1=S. W. |last2=Lattmer |first2=J. M. |last3=Margolis |first3=S. H. |year=1977 |title=Are supernovae sources of presolar grains? |journal=] |volume=270 |issue=5639 |pages=700–701 |bibcode=1977Natur.270..700F |doi=10.1038/270700a0 |s2cid=4240932}}</ref> This is suggested by a high ] of heavy elements in the Solar System, such as ] and ], relative to the abundances of these elements in so-called ], heavy-element-poor, stars. The heavy elements could most plausibly have been produced by ] nuclear reactions during a supernova, or by ] through ] within a massive second-generation star.<ref name="zeilik" />


The Sun is by far the ], with an ] of −26.74.<ref>{{Cite journal |last=Burton |first=W. B. |date=1986 |title=Stellar parameters |journal=] |volume=43 |issue=3–4 |pages=244–250 |doi=10.1007/BF00190626 |s2cid=189796439}}</ref><ref>{{Cite journal |last1=Bessell |first1=M. S. |last2=Castelli |first2=F. |last3=Plez |first3=B. |date=1998 |title=Model atmospheres broad-band colors, bolometric corrections and temperature calibrations for O–M stars |journal=] |volume=333 |pages=231–250 |bibcode=1998A&A...333..231B}}</ref> This is about 13&nbsp;billion times brighter than the next brightest star, ], which has an apparent magnitude of −1.46.<ref name="Hoffleit1991">{{cite book | chapter=HR 2491 | title=Bright Star Catalogue |edition= 5th Revised |last1=Hoffleit | first1=D. |author-link1=Dorrit Hoffleit |display-authors=etal | date=1991 | publisher=] | url=http://vizier.u-strasbg.fr/viz-bin/VizieR-S?HR%202491 |bibcode= 1991bsc..book.....H}}</ref>
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 a million ] while its visible surface (the ]) has a temperature of less than 6,000 K. Current topics of scientific inquiry include the Sun's regular cycle of ] activity, the physics and origin of ]s and ], the magnetic interaction between the ] and the ], and the origin of the ].


{{convert|1|AU|e6km e6mi|lk=in|spell=In|disp=x|abbr=off| (about |)}} is defined as the mean distance between the centers of the Sun and the Earth. The instantaneous distance varies by about {{±}}{{convert|2.5|e6km|abbr=none}} as Earth moves from ] around 3 January to ] around 4 July.<ref name="USNO">{{Cite web |date=31 January 2008 |title=Equinoxes, Solstices, Perihelion, and Aphelion, 2000–2020 |url=http://aa.usno.navy.mil/data/docs/EarthSeasons.php |url-status=live |archive-url=https://web.archive.org/web/20071013000301/http://aa.usno.navy.mil/data/docs/EarthSeasons.php |archive-date=13 October 2007 |access-date=17 July 2009 |publisher=]}}</ref> At its average distance, light travels from the Sun's horizon to Earth's horizon in about 8 minutes and 20 seconds,<ref>{{Cite web |last=Cain |first=Fraser |date=15 April 2013 |title=How long does it take sunlight to reach the Earth? |url=https://phys.org/news/2013-04-sunlight-earth.html |url-status=live |archive-url=https://web.archive.org/web/20220302095547/https://phys.org/news/2013-04-sunlight-earth.html |archive-date=2 March 2022 |access-date=2 March 2022 |website=phys.org}}</ref> while light from the closest points of the Sun and Earth takes about two seconds less. The energy of this ] supports almost all life<ref group="lower-alpha">] live so deep under the sea that they have no access to sunlight. Bacteria instead use sulfur compounds as an energy source, via ].</ref> on Earth by ],<ref>{{cite web |title=The Sun's Energy: An Essential Part of the Earth System |url=https://scied.ucar.edu/learning-zone/earth-system/energy-from-sun |website=Center for Science Education |access-date=24 May 2024}}</ref> and drives ] and weather.<ref>{{cite web |title=The Sun's Influence on Climate |url=https://press.princeton.edu/books/hardcover/9780691153834/the-suns-influence-on-climate |date=23 June 2015 |publisher=Princeton University Press |access-date=24 May 2024}}</ref>
== Life cycle ==


The Sun does not have a definite boundary, but its density decreases exponentially with increasing height above the ].<ref name="Beer et al, 2012-41">{{Cite book |last1=Beer |first1=J. |title=Cosmogenic Radionuclides: Theory and Applications in the Terrestrial and Space Environments |url=https://books.google.com/books?id=zKA0tZg0HwEC&pg=PA41 |last2=McCracken |first2=K. |last3=von Steiger |first3=R. |date=2012 |publisher=Springer |isbn=978-3-642-14651-0 |page=41}}</ref> For the purpose of measurement, the Sun's radius is considered to be the distance from its center to the edge of the photosphere, the apparent visible surface of the Sun.<ref name="Phillips1995-73">{{Cite book |last=Phillips |first=K. J. H. |title=Guide to the Sun |date=1995 |publisher=] |isbn=978-0-521-39788-9 |url=https://books.google.com/books?id=idwBChjVP0gC&pg=PA73 |page=73}}</ref>
The Sun's current age, determined using ] of ] and ], is thought to be about 4.57 billion years.<ref name="Bonanno">{{cite journal
The roundness of the Sun is relative difference between its radius at its equator, <math>R_\textrm{eq}</math>, and at its pole, <math>R_\textrm{pol}</math>, called the ],<ref name=Meftah-2015>{{Cite journal |last1=Meftah |first1=M. |last2=Irbah |first2=A. |last3=Hauchecorne |first3=A. |last4=Corbard |first4=T. |last5=Turck-Chièze |first5=S. |last6=Hochedez |first6=J.-F. |last7=Boumier |first7=P. |last8=Chevalier |first8=A. |last9=Dewitte |first9=S. |last10=Mekaoui |first10=S. |last11=Salabert |first11=D. |date=March 2015 |title=On the Determination and Constancy of the Solar Oblateness |url=http://link.springer.com/10.1007/s11207-015-0655-6 |journal=Solar Physics |language=en |volume=290 |issue=3 |pages=673–687 |doi=10.1007/s11207-015-0655-6 |bibcode=2015SoPh..290..673M |issn=0038-0938}}</ref>
|last=Bonanno
<math display="block">\Delta_\odot = (R_\textrm{eq} -R_\textrm{pol})/R_\textrm{pol}.</math>
|first=A.
The value is difficult to measure. Atmospheric distortion means the measurement must be done on satellites; the value is very small meaning very precise technique is needed.<ref name=GoughOverview2012>{{Cite journal |last=Gough |first=Douglas |date=2012-09-28 |title=How Oblate Is the Sun? |url=https://www.science.org/doi/10.1126/science.1226988 |journal=Science |language=en |volume=337 |issue=6102 |pages=1611–1612 |doi=10.1126/science.1226988 |bibcode=2012Sci...337.1611G |issn=0036-8075}}</ref>
|coauthors=Schlattl, H.; Patern, L.
|year= 2002
|url=http://arxiv.org/PS_cache/astro-ph/pdf/0204/0204331.pdf
|title=The age of the Sun and the relativistic corrections in the EOS
|journal=Astronomy and Astrophysics
|volume=390
|pages=1115-1118}}</ref>] The Sun is about halfway through its ] ], during which ] reactions in its core fuse hydrogen into helium. Each second, more than 4 million ]s of matter are converted into energy within the Sun's core, producing ]s and ]. The Sun will spend a total of approximately 10 ] years as a main sequence star.


The oblateness was once proposed to be sufficient to explain the ] but Einstein proposed that ] could explain the precession using a spherical Sun.<ref name=GoughOverview2012/> When high precision measurements of the oblateness became available via the ]<ref>{{Cite journal |last1=Kuhn |first1=J. R. |last2=Bush |first2=R. |last3=Emilio |first3=M. |last4=Scholl |first4=I. F. |date=2012-09-28 |title=The Precise Solar Shape and Its Variability |url=https://www.science.org/doi/10.1126/science.1223231 |journal=Science |language=en |volume=337 |issue=6102 |pages=1638–1640 |doi=10.1126/science.1223231 |bibcode=2012Sci...337.1638K |issn=0036-8075}}</ref> and the
The Sun does not have enough mass to explode as a ]. Instead, in 4-5 billion years, it will enter a ] 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 about 3{{e|8}}&nbsp;K. 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. However, Earth's water and most of the atmosphere will be boiled away.
] satellite<ref name=Meftah-2015/> the measured value was even smaller than expected,<ref name=GoughOverview2012/> 8.2 x 10<sup>-6</sup>, or 8 parts per million.
This makes the Sun the natural object closest to a perfect sphere.<ref name="perfect sphere">{{Cite web |last=Jones |first=G. |date=16 August 2012 |title=Sun is the most perfect sphere ever observed in nature |url=https://www.theguardian.com/science/2012/aug/16/sun-perfect-sphere-nature |url-status=live |archive-url=https://web.archive.org/web/20140303022045/http://www.theguardian.com/science/2012/aug/16/sun-perfect-sphere-nature |archive-date=3 March 2014 |access-date=19 August 2013 |website=]}}</ref> The oblateness value remains constant independent of solar irradiation changes.<ref name=Meftah-2015/> The tidal effect of the planets is weak and does not significantly affect the shape of the Sun.<ref name="Schutz2003">{{Cite book |last=Schutz |first=B. F. |title=Gravity from the ground up |url=https://books.google.com/books?id=P_T0xxhDcsIC&pg=PA98 |year=2003 |publisher=] |isbn=978-0-521-45506-0 |pages=98–99}}</ref>


===Rotation===
Following the red giant phase, intense thermal pulsations will cause the Sun to throw off its outer layers, forming a ]. The only object that remains after the outer layers are ejected is the extremely hot stellar core, which will slowly cool and fade as a ] over many billions of years. This ] scenario is typical of low- to medium-mass stars.<ref name="future-sun">{{cite web
{{main|Solar rotation}}
|author=Pogge, Richard W.
The Sun rotates faster at its equator than at its ]. This ] is caused by ] due to heat transport and the ] due to the Sun's rotation. In a frame of reference defined by the stars, the rotational period is approximately 25.6 days at the equator and 33.5 days at the poles. Viewed from Earth as it orbits the Sun, the ''apparent rotational period'' of the Sun at its equator is about 28 days.<ref name="Phillips1995-78">{{Cite book |last=Phillips |first=K. J. H. |title=Guide to the Sun |year=1995 |publisher=] |isbn=978-0-521-39788-9 |url=https://books.google.com/books?id=idwBChjVP0gC&pg=PA78 |pages=78–79}}</ref> Viewed from a vantage point above its north pole, the Sun rotates ] around its axis of spin.{{efn|name=rotation}}<ref name="spaceacademy">{{Cite web |title=The Anticlockwise Solar System |url=https://www.spaceacademy.net.au/library/notes/anticlok.htm |url-status=live |archive-url=https://web.archive.org/web/20200807081832/https://www.spaceacademy.net.au/library/notes/anticlok.htm |archive-date=7 August 2020 |access-date=2 July 2020 |publisher=Australian Space Academy}}</ref>
|year=1997
|url=http://www-astronomy.mps.ohio-state.edu/~pogge/Lectures/vistas97.html
|title=The Once & Future Sun
|format=lecture notes
|work=
|accessdate=2005-12-07}}</ref><ref name="Sackmann">{{cite journal
|last=Sackmann
|first=I.-Juliana
|coauthors=Arnold I. Boothroyd; Kathleen E. Kraemer
|year=1993
|month=11
|url=http://adsabs.harvard.edu/cgi-bin/nph-bib_query?1993ApJ%2E%2E%2E418%2E%2E457S&db_key=AST&high=24809&nosetcookie=1
|title=Our Sun. III. Present and Future
|journal=Astrophysical Journal
|volume=418
|pages=457}}</ref>


A survey of ]s suggest the early Sun was rotating up to ten times faster than it does today. This would have made the surface much more active, with greater X-ray and UV emission. Sun spots would have covered 5–30% of the surface.<ref>{{cite conference | title=The Sun in time: age, rotation, and magnetic activity of the Sun and solar-type stars and effects on hosted planets | last1=Guinan | first1=Edward F. | last2=Engle | first2=Scott G. | conference=The Ages of Stars, Proceedings of the International Astronomical Union, IAU Symposium | volume=258 | pages=395–408 | date=June 2009 | doi=10.1017/S1743921309032050 | arxiv=0903.4148 | bibcode=2009IAUS..258..395G }}</ref> The rotation rate was gradually slowed by ], as the Sun's magnetic field interacted with the outflowing solar wind.<ref>{{cite journal | title=Magnetic Braking of Sun-like and Low-mass Stars: Dependence on Coronal Temperature | last1=Pantolmos | first1=George | last2=Matt | first2=Sean P. | journal=The Astrophysical Journal | volume=849 | issue=2 | at=id. 83 | date=November 2017 | doi=10.3847/1538-4357/aa9061 | doi-access=free | arxiv=1710.01340 | bibcode=2017ApJ...849...83P }}</ref> A vestige of this rapid primordial rotation still survives at the Sun's core, which has been found to be rotating at a rate of once per week; four times the mean surface rotation rate.<ref>{{cite journal | title=Asymptotic g modes: Evidence for a rapid rotation of the solar core | last1=Fossat | first1=E. | last2=Boumier | first2=P. | last3=Corbard | first3=T. | last4=Provost | first4=J. | last5=Salabert | first5=D. | last6=Schmider | first6=F. X. | last7=Gabriel | first7=A. H. | last8=Grec | first8=G. | last9=Renaud | first9=C. | last10=Robillot | first10=J. M. | last11=Roca-Cortés | first11=T. | last12=Turck-Chièze | first12=S. | last13=Ulrich | first13=R. K. | last14=Lazrek | first14=M. | journal=Astronomy & Astrophysics | volume=604 | at=id. A40 | date=August 2017 | doi=10.1051/0004-6361/201730460 | arxiv=1708.00259 | bibcode=2017A&A...604A..40F }}</ref><ref>{{cite web | title=ESA, NASA's SOHO Reveals Rapidly Rotating Solar Core | first=Susannah | last=Darling | date=August 1, 2017 | publisher=] | url=https://www.nasa.gov/science-research/heliophysics/esa-nasas-soho-reveals-rapidly-rotating-solar-core/ | access-date=2024-05-31 }}</ref>
==Structure==
]
While the Sun is an averaged-sized star, it contains approximately 99% of the total mass of the solar system. The Sun is a near-perfect ], with an ] estimated at about 9 millionths,<ref name="Godier">{{cite journal
|last=Godier
|first=S.
|coauthors=Rozelot J.-P.
|year=2000
|url=http://aa.springer.de/papers/0355001/2300365.pdf
|title=The solar oblateness and its relationship with the structure of the tachocline and of the Sun's subsurface
|journal=Astronomy and Astrophysics
|volume=355
|pages=365-374}}</ref> which means that its polar diameter differs from its equatorial diameter by only 10&nbsp;km. While the Sun does not rotate as a solid body (the rotational period is 25 days at the ] and about 35 days at the ]), it takes approximately 28 days to complete one full rotation; the centrifugal effect of this slow ] is 18 million times weaker than the surface gravity at the Sun's equator. Tidal effects from the planets do not significantly affect the shape of the Sun, although the Sun itself orbits the ] of the solar system, which is located nearly a solar radius away from the center of the Sun mostly because of the large mass of ].


== Composition ==
The Sun does not have a definite boundary as rocky planets do; the density of its gases drops approximately ] 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 ]. This is simply the layer below which the gases are thick enough to be ] but above which they are ]; the photosphere is the surface most readily visible to the ]. Most of the Sun's mass lies within about 0.7 ] of the center.
{{See also|Molecules in stars}}
The Sun consists mainly of the elements ] and ]. At this time in the Sun's life, they account for 74.9% and 23.8%, respectively, of the mass of the Sun in the photosphere.<ref name=lodders>{{cite journal |doi=10.1086/375492 |last=Lodders |first=Katharina|author-link=Katharina Lodders |date=10 July 2003 |title=Solar System Abundances and Condensation Temperatures of the Elements |journal=The Astrophysical Journal |volume=591 |issue=2 |pages=1220–1247 |url=http://weft.astro.washington.edu/courses/astro557/LODDERS.pdf |bibcode=2003ApJ...591.1220L |access-date=1 September 2015 |archive-url=https://web.archive.org/web/20151107043527/http://weft.astro.washington.edu/courses/astro557/LODDERS.pdf |archive-date=7 November 2015 |url-status=dead |citeseerx=10.1.1.666.9351 |s2cid=42498829 }}<br />{{Cite journal |last=Lodders |first=K. |author-link=Katharina Lodders|title=Abundances and Condensation Temperatures of the Elements |url=http://www.lpi.usra.edu/meetings/metsoc2003/pdf/5272.pdf |journal=] |volume=38 |issue=suppl |page=5272 |date=2003 |bibcode=2003M&PSA..38.5272L |access-date=3 August 2008 |archive-date=13 May 2011 |archive-url=https://web.archive.org/web/20110513163004/http://www.lpi.usra.edu/meetings/metsoc2003/pdf/5272.pdf |url-status=live }}</ref> All heavier elements, called '']'' in astronomy, account for less than 2% of the mass, with ] (roughly 1% of the Sun's mass), ] (0.3%), ] (0.2%), and ] (0.2%) being the most abundant.<ref name=hkt2004>{{Cite book |last1=Hansen |first1=C. J. |last2=Kawaler |first2=S. A. |last3=Trimble |first3=V. |title=Stellar Interiors: Physical Principles, Structure, and Evolution |pages=19–20 |edition=2nd |publisher=] |date=2004 |isbn=978-0-387-20089-7}}</ref>


The Sun's original chemical composition was inherited from the ] out of which it formed. Originally it would have been about 71.1% hydrogen, 27.4% helium, and 1.5% heavier elements.<ref name=lodders /> The hydrogen and most of the helium in the Sun would have been produced by ] in the first 20 minutes of the universe, and the heavier elements were ] before the Sun was formed, and spread into the interstellar medium during the ] and by events such as ]e.<ref name="hkt2004_78">{{Cite book |last1=Hansen |first1=C. J. |title=Stellar Interiors: Physical Principles, Structure, and Evolution |last2=Kawaler |first2=S. A. |last3=Trimble |first3=V. |year=2004 |publisher=] |isbn=978-0-387-20089-7 |edition=2nd |pages=77–78}}</ref>
The solar interior is not directly observable, and the Sun itself is opaque to electromagnetic radiation. However, just as ] uses waves generated by ]s to reveal the interior structure of the Earth, the discipline of ] makes use of pressure waves (]) traversing the Sun's interior to measure and visualize the Sun's inner structure. ] of the Sun is also used as a theoretical tool to investigate its deeper layers.


Since the Sun formed, the main fusion process has involved fusing hydrogen into helium. Over the past 4.6&nbsp;billion years, the amount of helium and its location within the Sun has gradually changed. The proportion of helium within the core has increased from about 24% to about 60% due to fusion, and some of the helium and heavy elements have settled from the photosphere toward the center of the Sun because of ]. The proportions of heavier elements are unchanged. ] outward from the Sun's core by radiation rather than by convection (see ] below), so the fusion products are not lifted outward by heat; they remain in the core,<ref name=hkt2004_9.2.3>{{Cite book |last1=Hansen |first1=C. J. |last2=Kawaler |first2=S. A. |last3=Trimble |first3=V. |title=Stellar Interiors: Physical Principles, Structure, and Evolution |pages=§&nbsp;9.2.3 |no-pp=yes |edition=2nd |publisher=] |year=2004 |isbn=978-0-387-20089-7}}</ref> and gradually an inner core of helium has begun to form that cannot be fused because presently the Sun's core is not hot or dense enough to fuse helium. In the current photosphere, the helium fraction is reduced, and the ] is only 84% of what it was in the ] phase (before nuclear fusion in the core started). In the future, helium will continue to accumulate in the core, and in about 5&nbsp;billion years this gradual build-up will eventually cause the Sun to exit the ] and become a ].<ref>{{cite journal | last=Iben | first=Icko Jnr. | title=Stellar Evolution. II. The Evolution of a 3 M<sub>☉</sub> Star from the Main Sequence Through Core Helium Burning | journal=Astrophysical Journal | volume=142 | page=1447 | date=November 1965 | doi=10.1086/148429 | bibcode=1965ApJ...142.1447I }}</ref>
===Core===
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/m<sup>3</sup> (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 (1/2350<sup>th</sup> of the core)). Through most of the Sun's life, energy is produced by ] through a series of steps called the p-p (proton-proton) chain; this process converts ] into ]. The core is the only location in the Sun that produces an appreciable amount of ] 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 ] or ] of particles.


The chemical composition of the photosphere is normally considered representative of the composition of the primordial Solar System.<ref name="aller1968">{{Cite journal |last=Aller |first=L. H. |title=The chemical composition of the Sun and the solar system |journal=Proceedings of the Astronomical Society of Australia |volume=1 |issue=4 |page=133 |date=1968 |bibcode=1968PASA....1..133A|doi=10.1017/S1323358000011048|s2cid=119759834 |doi-access=free }}</ref> Typically, the solar heavy-element abundances described above are measured both by using ] of the Sun's photosphere and by measuring abundances in ] that have never been heated to melting temperatures. These meteorites are thought to retain the composition of the protostellar Sun and are thus not affected by the settling of heavy elements. The two methods generally agree well.<ref name="basu2008">{{Cite journal |last1=Basu |first1=S. |last2=Antia |first2=H. M. |year=2008 |title=Helioseismology and Solar Abundances |journal=] |volume=457 |issue=5–6 |pages=217–283 |arxiv=0711.4590 |bibcode=2008PhR...457..217B |doi=10.1016/j.physrep.2007.12.002 |s2cid=119302796}}</ref>
About 8.9{{e|37}} ]s (hydrogen nuclei) are converted into helium nuclei every second, releasing energy at the matter-energy conversion rate of 4.26 million tonnes per second, 383 ] (383{{e|24}} W) or 9.15{{e|10}} ]s of ] per second. The rate of nuclear fusion depends strongly on density, 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 ] slightly against the ] of the outer layers, reducing the fusion rate and correcting the ]; 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.


== Structure and fusion ==
The high-energy ]s (gamma and X-rays) released in fusion reactions take a long time to reach the Sun's surface, slowed down by the indirect path taken, as well as by constant absorption and reemission at lower energies in the solar mantle. Estimates of the "photon travel time" range from as much as 50 million years<ref name="Lewis">{{cite book
{{Main|Standard solar model}}
|last=Lewis
]
|first=Richard
{{Clear}}
|year=1983
|title=The Illustrated Encyclopedia of the Universe
|publisher=Harmony Books, New York
|pages=65}}</ref> to as little as 17,000 years.<ref name="Bad Astronomy">{{cite web
|url=http://www.badastronomy.com/bitesize/solar_system/sun.html
|first=Phil
|last=Plait
|publisher=Bad Astronomy
|title=Bitesize Tour of the Solar System: The Long Climb from the Sun's Core
|year=1997
|accessdate=2006-03-22}}</ref> After a final trip through the convective outer layer to the transparent "surface" of the photosphere, the photons escape as ]. Each gamma ray in the Sun's core is converted into several million visible light photons before escaping into space. ]s are also released by the fusion reactions in the core, but unlike photons they very 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 ], a problem which was recently resolved through a better understanding of the effects of ].


===Radiation zone=== === Core ===
{{Main|Solar core}}
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 ]; while the material grows cooler as altitude increases, this temperature ] is slower than the ] and hence cannot drive convection. Heat is transferred by ]&mdash;] of hydrogen and helium emit ], which travel a brief distance before being reabsorbed by other ions.
The core of the Sun extends from the center to about 20–25% of the solar radius.<ref name="Garcia2007">{{Cite journal |last=García |first=R. |date=2007 |title=Tracking solar gravity modes: the dynamics of the solar core |journal=] |volume=316 |issue=5831 |pages=1591–1593 |bibcode=2007Sci...316.1591G |doi=10.1126/science.1140598 |pmid=17478682 |s2cid=35285705|display-authors=etal }}</ref> It has a density of up to {{val|150|u=g|up=cm3}}<ref name="Basu">{{Cite journal | last1=Basu | first1=Sarbani | last2=Chaplin | first2=William J. | last3=Elsworth | first3=Yvonne | last4=New | first4=Roger | last5=Serenelli | first5=Aldo M. |year=2009 |title=Fresh insights on the structure of the solar core |journal=] |volume=699 |issue=2 |pages=1403–1417 |arxiv=0905.0651 |bibcode=2009ApJ...699.1403B |doi=10.1088/0004-637X/699/2/1403|s2cid=11044272 }}</ref><ref name="NASA1">{{Cite web |date=18 January 2007 |title=NASA/Marshall Solar Physics |url=http://solarscience.msfc.nasa.gov/interior.shtml |url-status=live |archive-url=https://web.archive.org/web/20190329081742/https://solarscience.msfc.nasa.gov/interior.shtml |archive-date=29 March 2019 |access-date=11 July 2009 |publisher=]}}</ref> (about 150 times the density of water) and a temperature of close to 15.7&nbsp;million ] (K).<ref name="NASA1" /> By contrast, the Sun's surface temperature is about {{val|5,800|u=K}}. Recent analysis of ] mission data favors the idea that the core is rotating faster than the radiative zone outside it.<ref name="Garcia2007" /> Through most of the Sun's life, energy has been produced by nuclear fusion in the core region through the ]; this process converts hydrogen into helium.<ref>{{Cite conference |last=Broggini |first=C. |date=2003 |title=Physics in Collision, Proceedings of the XXIII International Conference: Nuclear Processes at Solar Energy |url=http://www.slac.stanford.edu/econf/C030626 |conference=XXIII Physics in Collisions Conference |location=Zeuthen, Germany |page=21 |arxiv=astro-ph/0308537 |bibcode=2003phco.conf...21B |archive-url=https://web.archive.org/web/20170421113407/http://www.slac.stanford.edu/econf/C030626/ |archive-date=21 April 2017 |access-date=12 August 2013 |url-status=live}}</ref> Currently, 0.8% of the energy generated in the Sun comes from another sequence of fusion reactions called the ]; the proportion coming from the CNO cycle is expected to increase as the Sun becomes older and more luminous.<ref name="jpcs271_1_012031">{{Cite journal |last1=Goupil |first1=M. J. |last2=Lebreton |first2=Y. |last3=Marques |first3=J. P. |last4=Samadi |first4=R. |last5=Baudin |first5=F. |date=2011 |title=Open issues in probing interiors of solar-like oscillating main sequence stars 1. From the Sun to nearly suns |journal=] |volume=271 |issue=1 |page=012031 |arxiv=1102.0247 |bibcode=2011JPhCS.271a2031G |doi=10.1088/1742-6596/271/1/012031|s2cid=4776237 }}</ref><ref>{{Cite journal |last=The Borexino Collaboration |date=2020 |title=Experimental evidence of neutrinos produced in the CNO fusion cycle in the Sun |url=https://www.nature.com/articles/s41586-020-2934-0 |journal=] |volume=587 |issue=? |pages=577–582 |arxiv=2006.15115 |bibcode=2020Natur.587..577B |doi=10.1038/s41586-020-2934-0 |pmid=33239797 |s2cid=227174644 |access-date=26 November 2020 |archive-date=27 November 2020 |archive-url=https://web.archive.org/web/20201127093809/https://www.nature.com/articles/s41586-020-2934-0 |url-status=live }}</ref>


The core is the only region of the Sun that produces an appreciable amount of ] through fusion; 99% of the Sun's power is generated in the innermost 24% of its radius, and almost no fusion occurs beyond 30% of the radius. The rest of the Sun is heated by this energy as it is transferred outward through many successive layers, finally to the solar photosphere where it escapes into space through radiation (photons) or advection (massive particles).<ref name="Phillips1995-47">{{Cite book |last=Phillips |first=K. J. H. |title=Guide to the Sun |year=1995 |publisher=] |isbn=978-0-521-39788-9 |url=https://books.google.com/books?id=idwBChjVP0gC&pg=PA47 |pages=47–53}}</ref><ref name=Zirker2002-15>{{Cite book |last=Zirker |first=J. B. |date=2002 |title=Journey from the Center of the Sun |pages= |publisher=] |isbn=978-0-691-05781-1 |url=https://archive.org/details/journeyfromcente0000zirk/page/15 }}</ref>
===Convection zone===
], ], and regular ]|alt=circles and arrows showing protons combining in a series of fusion reactions yielding helium-3 which breaks down tow helium-4]]
]
The proton–proton chain occurs around {{val|9.2|e=37}} times each second in the core, converting about 3.7{{e|38}} protons into ]s (helium nuclei) every second (out of a total of ~8.9{{e|56}} free protons in the Sun), or about {{val|6.2|e=11|u=kg|up=s}}. However, each proton (on average) takes around 9 billion years to fuse with another using the PP chain.<ref name="Phillips1995-47" /> Fusing four free ]s (hydrogen nuclei) into a single alpha particle (helium nucleus) releases around 0.7% of the fused mass as energy,<ref>{{Cite book |last=Shu |first=F. H. |url=https://archive.org/details/physicaluniverse00shuf/page/102 |title=The Physical Universe: An Introduction to Astronomy |year=1982 |publisher=University Science Books |isbn=978-0-935702-05-7 |page=}}</ref> so the Sun releases energy at the mass–energy conversion rate of 4.26&nbsp;billion kg/s (which requires 600 billion kg of hydrogen<ref>{{Cite web |year=2012 |title=Ask Us: Sun |url=https://helios.gsfc.nasa.gov/qa_sun.html |url-status=dead |archive-url=https://web.archive.org/web/20180903223810/https://helios.gsfc.nasa.gov/qa_sun.html |archive-date=3 September 2018 |access-date=13 July 2017 |website=Cosmicopia |publisher=NASA}}</ref>), for 384.6&nbsp;] ({{val|3.846|e=26|u=W}}),<ref name="nssdc" /> or 9.192{{e|10}}&nbsp;] per second. The large power output of the Sun is mainly due to the huge size and density of its core (compared to Earth and objects on Earth), with only a fairly small amount of power being generated per ]. Theoretical models of the Sun's interior indicate a maximum power density, or energy production, of approximately 276.5 ]s per cubic metre at the center of the core,<ref>{{Cite web |last=Cohen |first=H. |date=9 November 1998 |title=Table of temperatures, power densities, luminosities by radius in the Sun |url=http://fusedweb.llnl.gov/CPEP/Chart_Pages/5.Plasmas/Sunlayers.html |archive-url=http://webarchive.loc.gov/all/20011129122524/http%3A//fusedweb%2Ellnl%2Egov/cpep/chart_pages/5%2Eplasmas/sunlayers%2Ehtml |archive-date=29 November 2001 |access-date=30 August 2011 |publisher=Contemporary Physics Education Project}}</ref> which, according to ], is about the same power density inside a ].<ref>{{Cite web |date=17 April 2012 |title=Lazy Sun is less energetic than compost |url=http://www.abc.net.au/science/articles/2012/04/17/3478276.htm |url-status=live |archive-url=https://web.archive.org/web/20140306123113/http://www.abc.net.au/science/articles/2012/04/17/3478276.htm |archive-date=6 March 2014 |access-date=25 February 2014 |website=]}}</ref>


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 ] slightly against the weight of the outer layers, reducing the density and hence the fusion rate and correcting the ]; and a slightly lower rate would cause the core to cool and shrink slightly, increasing the density and increasing the fusion rate and again reverting it to its present rate.<ref>{{Cite journal |last1=Haubold |first1=H. J. |last2=Mathai |first2=A. M. |date=1994 |title=Solar Nuclear Energy Generation & The Chlorine Solar Neutrino Experiment |volume=320 |issue=1994 |pages=102–116 |journal=] |arxiv=astro-ph/9405040 |bibcode=1995AIPC..320..102H |doi=10.1063/1.47009|citeseerx=10.1.1.254.6033|s2cid=14622069 }}</ref><ref>{{Cite web |last=Myers |first=S. T. |date=18 February 1999 |title=Lecture 11 – Stellar Structure I: Hydrostatic Equilibrium |url=http://www.aoc.nrao.edu/~smyers/courses/astro12/L11.html |url-status=live |archive-url=https://web.archive.org/web/20110512180052/http://www.aoc.nrao.edu/~smyers/courses/astro12/L11.html |archive-date=12 May 2011 |access-date=15 July 2009 |website=Introduction to Astrophysics II}}</ref>
From about 0.7 solar radii to the Sun's visible surface, the material in the Sun 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 ] 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 radiative zone. ] is thought to occur at the base of the convection zone, carrying turbulent downflows into the outer layers of the radiative zone.


=== Radiative zone ===
The thermal columns in the convection zone form an imprint on the surface of the Sun, in the form of the ] and ]. 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.
{{Main|Radiative zone}}
]
The radiative zone is the thickest layer of the Sun, at 0.45 solar radii. From the core out to about 0.7 ], ] is the primary means of energy transfer.<ref name="autogenerated1">{{cite web |url=http://mynasa.nasa.gov/worldbook/sun_worldbook.html |publisher=NASA |title=Sun |website=World Book at NASA |access-date=10 October 2012 |url-status=dead |archive-url=https://web.archive.org/web/20130510142009/http://mynasa.nasa.gov/worldbook/sun_worldbook.html |archive-date=10 May 2013}}</ref> The temperature drops from approximately 7&nbsp;million to 2&nbsp;million kelvins with increasing distance from the core.<ref name="NASA1" /> This ] is less than the value of the ] and hence cannot drive convection, which explains why the transfer of energy through this zone is by ] instead of thermal convection.<ref name="NASA1" /> ] of hydrogen and helium emit photons, which travel only a brief distance before being reabsorbed by other ions.<ref name="autogenerated1" /> The density drops a hundredfold (from 20,000&nbsp;kg/m<sup>3</sup> to 200&nbsp;kg/m<sup>3</sup>) between 0.25 solar radii and 0.7 radii, the top of the radiative zone.<ref name="autogenerated1" /><!-- http://adsabs.harvard.edu/abs/2008SoPh..251..101M -->


===Photosphere=== === Tachocline ===
{{Main|Tachocline}}
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 because of the decreasing overall particle density: the photosphere is actually tens to hundreds of kilometers thick, being slightly less opaque than ] on Earth. Sunlight has approximately a ] spectrum that indicates its temperature is about 6,000 ] (10,340°F / 5,727&nbsp;°C), interspersed with atomic ]s from the tenuous layers above the photosphere. The photosphere has a particle density of about 10<sup>23</sup>&nbsp;m<sup>&minus;3</sup> (this is about 1% of the particle density of ] at sea level).


The radiative zone and the convective zone are separated by a transition layer, the ]. This is a region where the sharp regime change between the uniform rotation of the radiative zone and the differential rotation of the ] results in a large ] between the two—a condition where successive horizontal layers slide past one another.<ref>{{Cite book |last=Tobias |first=S. M. |title=Fluid Dynamics and Dynamos in Astrophysics and Geophysics |date=2005 |publisher=] |isbn=978-0-8493-3355-2 |editor-first=A. M. | editor-last=Soward |pages=193–235 |chapter=The solar tachocline: Formation, stability and its role in the solar dynamo |access-date=22 August 2020 |display-editors=etal |chapter-url=https://books.google.com/books?id=PLNwoJ6qFoEC&pg=PA193 |archive-url=https://web.archive.org/web/20201029102001/https://books.google.com/books?id=PLNwoJ6qFoEC&pg=PA193 |archive-date=29 October 2020 |url-status=live}}</ref> Presently, it is hypothesized that a magnetic dynamo, or ], within this layer generates the Sun's ].<ref name=NASA1 />
During early studies of the ] of the photosphere, some absorption lines were found that did not correspond to any ]s then known on Earth. In 1868, ] hypothesized that these absorption lines were because of a new element which he dubbed "]", after the Greek Sun god ]. It was not until 25 years later that helium was isolated on Earth.<ref name="Lockyer">{{cite web
|url=http://www-solar.mcs.st-andrews.ac.uk/~clare/Lockyer/helium.html
|title=Discovery of Helium
|accessdate=2006-03-22}}</ref>


===Atmosphere=== === Convective zone ===
{{Main|Convection zone}}
], the Sun's atmosphere is more apparent to the eye.]]
The Sun's convection zone extends from 0.7 solar radii (500,000&nbsp;km) to near the surface. In this layer, the solar plasma is not dense or hot enough to transfer the heat energy of the interior outward via radiation. Instead, the density of the plasma is low enough to allow convective currents to develop and move the Sun's energy outward towards its surface. Material heated at the tachocline picks up heat and expands, thereby reducing its density and allowing it to rise. As a result, an orderly motion of the mass develops into thermal cells that carry most of the heat outward to the Sun's photosphere above. Once the material diffusively and radiatively cools just beneath the photospheric surface, its density increases, and it sinks to the base of the convection zone, where it again picks up heat from the top of the radiative zone and the convective cycle continues. At the photosphere, the temperature has dropped 350-fold to {{convert|5,700|K|F}} and the density to only 0.2&nbsp;g/m<sup>3</sup> (about 1/10,000 the density of air at sea level, and 1 millionth that of the inner layer of the convective zone).<ref name=NASA1 />


The thermal columns of the convection zone form an imprint on the surface of the Sun giving it a granular appearance called the ] at the smallest scale and ] at larger scales. Turbulent convection in this outer part of the solar interior sustains "small-scale" dynamo action over the near-surface volume of the Sun.<ref name=NASA1 /> The Sun's thermal columns are ] and take the shape of roughly hexagonal prisms.<ref>{{Cite book |last=Mullan |first=D. J. |title=From the Sun to the Great Attractor |year=2000 |publisher=] |isbn=978-3-540-41064-5 |editor-last=Page | editor-first=D. |page=22 |chapter=Solar Physics: From the Deep Interior to the Hot Corona |access-date=22 August 2020 |editor-last2=Hirsch |editor-first2=J. G. |chapter-url=https://books.google.com/books?id=rk5fxs55_OkC&pg=PA22 |archive-url=https://web.archive.org/web/20210417080656/https://books.google.com/books?id=rk5fxs55_OkC&pg=PA22 |archive-date=17 April 2021 |url-status=live}}</ref>
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 ], from radio through ] to ], and comprise five principal zones: the ''temperature minimum'', the ], the ], the ], and the ]. The heliosphere, which may be considered the tenuous outer atmosphere of the Sun, extends outward past the orbit of ] to the ], where it forms a sharp ] boundary with the ]. The chromosphere, transition region, and corona are much hotter than the surface of the Sun; the reason why is not yet known.


=== Photosphere ===
The coolest layer of the Sun is a temperature minimum region about 500&nbsp;km above the photosphere, with a temperature of about 4,000&nbsp;]. This part of the Sun is cool enough to support simple molecules such as ] and water, which can be detected by their absorption spectra.
{{Main|Photosphere}}
]


The visible surface of the Sun, the photosphere, is the layer below which the Sun becomes ] to visible light.<ref name=Abhyankar1977 /> Photons produced in this layer escape the Sun through the transparent solar atmosphere above it and become solar radiation, sunlight. The change in opacity is due to the decreasing amount of ], which absorb visible light easily.<ref name=Abhyankar1977 /> Conversely, the visible light perceived is produced as electrons react with hydrogen atoms to produce H<sup>−</sup> ions.<ref name="Gibson">{{Cite book |last=Gibson |first=Edward G. |date=1973 |title=The Quiet Sun (NASA SP-303) |publisher=NASA |asin=B0006C7RS0}}</ref><ref name="Shu">{{Cite book |last=Shu |first=F. H. |title=The Physics of Astrophysics |volume=1 |publisher=University Science Books |year=1991 |isbn=978-0-935702-64-4}}</ref>
Above the temperature minimum layer is a thin layer about 2,000&nbsp;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 ]. The temperature in the chromosphere increases gradually with altitude, ranging up to around 100,000&nbsp;K near the top.


The photosphere is tens to hundreds of kilometers thick, and is 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 '']''.<ref name="Abhyankar1977" /> The spectrum of sunlight has approximately the spectrum of a ] radiating at {{convert|5,772|K|F}},<ref name="IAU2015resB3"/> interspersed with atomic ]s from the tenuous layers above the photosphere. The photosphere has a particle density of ~10<sup>23</sup>&nbsp;m<sup>−3</sup> (about 0.37% of the particle number per volume of ] at sea level). The photosphere is not fully ionized—the extent of ionization is about 3%, leaving almost all of the hydrogen in atomic form.<ref>{{cite journal |last1=Rast |first1=M. |last2=Nordlund |first2=Å. |last3=Stein |first3=R. |last4=Toomre |first4=J. |date=1993 |title=Ionization Effects in Three-Dimensional Solar Granulation Simulations |journal=] |volume=408 |issue=1 |page=L53–L56 |bibcode=1993ApJ...408L..53R |doi=10.1086/186829|doi-access=free }}</ref>
Above the chromosphere is a ] in which the temperature rises rapidly from around 100,000&nbsp;] to coronal temperatures closer to one million K. The increase is because of a ] as ] within the region becomes fully ] by the high temperatures. The transition region does not occur at a well-defined altitude. Rather, it forms a kind of ] around chromospheric features such as ]s and ]s, and is in constant, chaotic motion. The transition region is not easily visible from Earth's surface, but is readily observable from ] by instruments sensitive to the ] portion of the ].


=== Atmosphere ===
The corona is the extended outer atmosphere of the Sun, which is much larger in volume than the Sun itself. The corona merges smoothly with the ] that fills the ] and ]. The low corona, which is very near the surface of the Sun, has a particle density of 10<sup>14</sup>&nbsp;m<sup>&minus;3</sup>&ndash;10<sup>16</sup>&nbsp;m<sup>&minus;3</sup>. (Earth's atmosphere near sea level has a particle density of about 2{{e|25}}&nbsp;m<sup>&minus;3</sup>.) The temperature of the corona is several million kelvin. While no complete theory yet exists to account for the temperature of the corona, at least some of its heat is known to be from ].
{{Main|Stellar atmosphere}}


The Sun's atmosphere is composed of five layers: the photosphere, the ], the ], the ], and the ].
The ] extends from approximately 20 solar radii (0.1&nbsp;AU) to the outer fringes of the solar system. Its inner boundary is defined as the layer in which the flow of the ] becomes ''superalfvénic''&mdash;that is, where the flow becomes faster than the speed of ]. Turbulence and dynamic forces outside this boundary cannot affect the shape of the solar corona within, because the information can only travel at the speed of Alfvén waves. The solar wind travels outward continuously through the heliosphere, forming the solar magnetic field into a ] shape, until it impacts the ] more than 50 AU from the Sun. In December 2004, the ] passed through a ] that is thought to be part of the heliopause. Both of the Voyager probes have recorded higher levels of energetic particles as they approach the boundary.<ref>{{cite web
|url=http://www.spaceref.com/news/viewpr.html?pid=16394
|title=The Distortion of the Heliosphere: our Interstellar Magnetic Compass
|month=March 15
|year=2005
|author=European Space Agency
|accessdate=2006-03-22}}</ref>


The coolest layer of the Sun is a temperature minimum region extending to about {{val|500|u=km}} above the photosphere, and has a temperature of about {{val|4100|ul=K|fmt=commas}}.<ref name="Abhyankar1977">{{Cite journal |last=Abhyankar |first=K. D. |date=1977 |title=A Survey of the Solar Atmospheric Models |url=http://prints.iiap.res.in/handle/2248/510 |url-status=live |journal=] |volume=5 |pages=40–44 |bibcode=1977BASI....5...40A |archive-url=https://web.archive.org/web/20200512151641/http://prints.iiap.res.in/handle/2248/510 |archive-date=12 May 2020 |access-date=12 July 2009}}</ref> This part of the Sun is cool enough to allow for the existence of simple molecules such as ] and water.<ref name="Solanki1994">{{Cite journal |last1=Solanki |first1=S. K. |last2=Livingston |first2=W. |last3=Ayres |first3=T. |date=1994 |title=New Light on the Heart of Darkness of the Solar Chromosphere |journal=] |pmid=17748350 |volume=263 |issue=5143 |pages=64–66 |bibcode=1994Sci...263...64S |doi=10.1126/science.263.5143.64 |s2cid=27696504 }}</ref> The chromosphere, transition region, and corona are much hotter than the surface of the Sun.<ref name="Abhyankar1977" /> The reason is not well understood, but evidence suggests that ]s may have enough energy to heat the corona.<ref>{{Cite journal |last=De Pontieu |first=B. |date=2007 |title=Chromospheric Alfvénic Waves Strong Enough to Power the Solar Wind |journal=] |volume=318 |issue=5856 |pages=1574–1577 |bibcode=2007Sci...318.1574D |doi=10.1126/science.1151747 |pmid=18063784 |s2cid=33655095|display-authors=etal}}</ref>
==Solar activity==
===Sunspots and the solar cycle===
]
When observing the Sun with appropriate filtration, the most immediately visible features are usually its ]s, which are well-defined surface areas that appear darker than their surroundings because of lower temperatures. Sunspots are regions of intense magnetic activity where ] is inhibited by strong magnetic fields, reducing energy transport from the hot interior to the surface. The magnetic field gives rise to strong heating in the corona, forming ]s that are the source of intense ]s and ]s. The largest sunspots can be tens of thousands of kilometers across.
]


]'s Solar Optical Telescope|left|alt=A photograph of the surface of the sun, with flares terminating from the surface on the left.]]
The number of sunspots visible on the Sun is not constant, but varies over a 10-12 year cycle known as the ]. At a typical solar minimum, few sunspots are visible, and occasionally none at all can be seen. Those that do appear are at high solar latitudes. As the sunspot cycle progresses, the number of sunspots increases and they move closer to the equator of the Sun, a phenomenon described by ]. Sunspots usually exist as pairs with opposite magnetic polarity. The polarity of the leading sunspot alternates every solar cycle, so that it will be a north magnetic pole in one solar cycle and a south magnetic pole in the next.


Above the temperature minimum layer is a layer about {{val|2000|u=km|fmt=commas}} thick, dominated by a spectrum of emission and absorption lines.<ref name="Abhyankar1977" /> 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 solar eclipses.<ref name="autogenerated1" /> The temperature of the chromosphere increases gradually with altitude, ranging up to around {{val|20000|u=K|fmt=commas}} near the top.<ref name="Abhyankar1977" /> In the upper part of the chromosphere helium becomes partially ].<ref name="Hansteen1997">{{Cite journal |last1=Hansteen |first1=V. H. |last2=Leer |first2=E. |last3=Holzer |first3=T. E. |date=1997 |title=The role of helium in the outer solar atmosphere |journal=] |volume=482 |issue=1 |pages=498–509 |bibcode=1997ApJ...482..498H |doi=10.1086/304111|doi-access=free }}</ref>
]
The solar cycle has a great influence on ], and seems also to have a strong influence on the Earth's climate. Solar minima tend to be correlated with colder temperatures, and longer than average solar cycles tend to be correlated with hotter temperatures. In the 17th century, the solar cycle appears to have stopped entirely for several decades; very few sunspots were observed during this period. During this era, which is known as the ] or ], Europe experienced very cold temperatures.<ref name="Lean">{{cite journal
|last=Lean
|first=J.
|coauthors=Skumanich A.; White O.
|year=1992
|title=Estimating the Sun's radiative output during the Maunder Minimum
|journal=Geophysical Research Letters
|volume=19
|pages=1591-1594}}</ref> Earlier extended minima have been discovered through analysis of ]s and also appear to have coincided with lower-than-average global temperatures.


Above the chromosphere, in a thin (about {{val|200|u=km}}) transition region, the temperature rises rapidly from around {{val|20000|u=K|fmt=commas}} in the upper chromosphere to coronal temperatures closer to {{val|1000000|u=K|fmt=commas}}.<ref name="Erdelyi2007">{{Cite journal |last1=Erdèlyi |first1=R. |last2=Ballai |first2=I. |date=2007 |title=Heating of the solar and stellar coronae: a review |journal=Astron. Nachr. |volume=328 |issue=8 |pages=726–733 |bibcode=2007AN....328..726E |doi=10.1002/asna.200710803 |doi-access=free}}</ref> The temperature increase is facilitated by the full ionization of helium in the transition region, which significantly reduces radiative cooling of the plasma.<ref name="Hansteen1997" /> The transition region does not occur at a well-defined altitude, but forms a kind of ] around chromospheric features such as ] and ], and is in constant, chaotic motion.<ref name="autogenerated1" /> The transition region is not easily visible from Earth's surface, but is readily observable from ] by instruments sensitive to ].<ref name="Dwivedi2006">{{Cite journal |last=Dwivedi |first=B. N. |date=2006 |title=Our ultraviolet Sun |url=http://www.iisc.ernet.in/currsci/sep102006/587.pdf |url-status=live |journal=] |volume=91 |issue=5 |pages=587–595 |archive-url=https://web.archive.org/web/20201025001339/http://www.iisc.ernet.in/currsci/sep102006/587.pdf |archive-date=25 October 2020 |access-date=22 March 2015}}</ref>
===Effects on Earth===
Solar activity has several effects on the Earth and its surroundings. Because the Earth has a magnetic field, charged particles from the solar wind cannot impact the atmosphere directly, but are instead deflected by the magnetic field and aggregate to form the ]. The Van Allen belts consist of an inner belt composed primarily of ]s and an outer belt composed mostly of ]s. Radiation within the Van Allen belts can occasionally damage ]s passing through them.


] the solar corona can be seen with the naked eye during totality.|alt=A photograph of a solar eclipse]]
The Van Allen belts form arcs around the Earth with their tips near the north and south poles. The most energetic particles can 'leak out' of the belts and strike the Earth's upper atmosphere, causing auroras, known as '']'' in the ] and ''aurorae australis'' in the ]. In periods of normal solar activity, aurorae can be seen in oval-shaped regions centered on the ]s and lying roughly at a ] of 65°, but at times of high solar activity the auroral oval can expand greatly, moving towards the equator. Aurorae borealis have been observed from locales as far south as ].


The corona is the next layer of the Sun. The low corona, near the surface of the Sun, has a particle density around 10<sup>15</sup>&nbsp;m<sup>−3</sup> to 10<sup>16</sup>&nbsp;m<sup>−3</sup>.<ref name=Hansteen1997 />{{efn|name=particle density}} The average temperature of the corona and solar wind is about 1,000,000–2,000,000&nbsp;K; however, in the hottest regions it is 8,000,000–20,000,000 K.<ref name=Erdelyi2007 /> Although no complete theory yet exists to account for the temperature of the corona, at least some of its heat is known to be from ].<ref name=Erdelyi2007 /><ref name="Russell2001">{{Cite book |last=Russell |first=C. T. |title=Space Weather (Geophysical Monograph) |date=2001 |publisher=] |isbn=978-0-87590-984-4 |editor-last=Song | editor-first=Paul |pages=73–88 |chapter=Solar wind and interplanetary magnetic filed: A tutorial |access-date=11 July 2009 |editor-last2=Singer | editor-first2=Howard J. |editor-last3=Siscoe | editor-first3=George L. |editor-link3=George Siscoe |chapter-url=http://www-ssc.igpp.ucla.edu/personnel/russell/papers/SolWindTutorial.pdf |archive-url=https://web.archive.org/web/20181001131951/http://www-ssc.igpp.ucla.edu/personnel/russell/papers/SolWindTutorial.pdf |archive-date=1 October 2018 |url-status=live}}</ref>
==Theoretical problems==
The corona is the extended atmosphere of the Sun, which has a volume much larger than the volume enclosed by the Sun's photosphere. A flow of plasma outward from the Sun into ] is the ].<ref name=Russell2001 />
===Solar neutrino problem===
]).]]


The heliosphere, the tenuous outermost atmosphere of the Sun, is filled with solar wind plasma and is defined to begin at the distance where the flow of the solar wind becomes ''superalfvénic''—that is, where the flow becomes faster than the speed of Alfvén waves,<ref>{{Cite book |last1=Emslie |first1=A. G. |last2=Miller |first2=J. A. |year=2003 |chapter=Particle Acceleration |chapter-url=https://books.google.com/books?id=W_oZYFplXX0C&pg=PA275 |editor-last=Dwivedi |editor-first=B. N. |title=Dynamic Sun |page=275 |publisher=] |isbn=978-0-521-81057-9}}</ref> at approximately 20 solar radii ({{val|0.1|u=AU}}). Turbulence and dynamic forces in the heliosphere cannot affect the shape of the solar corona within, because the information can only travel at the speed of Alfvén waves. The solar wind travels outward continuously through the heliosphere,<ref>{{Cite web |date=22 April 2003 |title=A Star with two North Poles |url=https://science.nasa.gov/headlines/y2003/22apr_currentsheet.htm |url-status=dead |archive-url=https://web.archive.org/web/20090718014855/https://science.nasa.gov/headlines/y2003/22apr_currentsheet.htm |archive-date=18 July 2009 |website=Science @ NASA |publisher=NASA}}</ref><ref>{{Cite journal |last1=Riley |first1=P. |last2=Linker |first2=J. A. |last3=Mikić |first3=Z. |date=2002 |title=Modeling the heliospheric current sheet: Solar cycle variations |journal=] |volume=107 |issue=A7 |pages=SSH 8–1 |bibcode=2002JGRA..107.1136R |doi=10.1029/2001JA000299 |id=CiteID 1136 |doi-access=free}}</ref> forming the solar magnetic field into a ] shape,<ref name=Russell2001 /> until it impacts the ] more than {{val|50|u=AU}} from the Sun. In December 2004, the '']'' probe passed through a shock front that is thought to be part of the heliopause.<ref>{{Cite press release |title=The Distortion of the Heliosphere: Our Interstellar Magnetic Compass |date=2005 |publisher=] |url=http://www.spaceref.com/news/viewpr.html?pid=16394 |access-date=22 March 2006 |url-status=live |archive-url=https://archive.today/20120604110953/http://www.spaceref.com/news/viewpr.html?pid=16394 |archive-date=4 June 2012}}</ref> In late 2012, ''Voyager 1'' recorded a marked increase in ] collisions and a sharp drop in lower energy particles from the solar wind, which suggested that the probe had passed through the heliopause and entered the ],<ref>{{Cite press release |last=Landau | first=Elizabeth|url=https://voyager.jpl.nasa.gov/news/details.php?article_id=44|title=Voyager 1 Helps Solve Interstellar Medium Mystery|publisher=]|date=October 29, 2015|url-status=live|archive-url=https://web.archive.org/web/20230803125531/https://voyager.jpl.nasa.gov/news/details.php?article_id=44|archive-date=August 3, 2023}}</ref> and indeed did so on August 25, 2012, at approximately 122 astronomical units (18&nbsp;Tm) from the Sun.<ref>{{Cite web|url=https://voyager.jpl.nasa.gov/mission/interstellar-mission/|title=Interstellar Mission|publisher=]|access-date=14 May 2021|archive-date=14 September 2017|archive-url=https://web.archive.org/web/20170914060928/https://voyager.jpl.nasa.gov/mission/interstellar-mission/#:~:text=On%20Aug.,billion%20kilometers)%20from%20the%20sun.|url-status=live}}</ref> The heliosphere has a ] which stretches out behind it due to the Sun's ] through the galaxy.<ref>{{cite web |last1=Dunbar |first1=Brian |title=Components of the Heliosphere |url=https://www.nasa.gov/mission_pages/sunearth/science/heliosphere-components.html |website=NASA |date=2 March 2015 |access-date=20 March 2021 |archive-date=8 August 2021 |archive-url=https://web.archive.org/web/20210808183941/https://www.nasa.gov/mission_pages/sunearth/science/heliosphere-components.html |url-status=live }}</ref>
For many years the number of solar ]s detected on Earth was only a third of the number expected, according to theories describing the nuclear reactions in the Sun. This anomalous result was termed the ]. Theories proposed to resolve the problem either tried to reduce the temperature of the Sun's interior to explain the lower neutrino flux, or posited that electron neutrinos could ], that is, change into undetectable ] and ]s as they traveled between the Sun and the Earth.<ref name="Haxton">{{cite journal
|last=Haxton
|first=W. C.
|year=1995
|url=http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1995ARA%26A..33..459H&amp;data_type=PDF_HIGH&amp;type=PRINTER&amp;filetype=.pdf
|title=The Solar Neutrino Problem
|journal=Annual Review of Astronomy and Astrophysics
|volume=33
|pages=459-504}}</ref> Several neutrino observatories were built in the 1980s to measure the solar neutrino flux as accurately as possible, including the ] and ]. Results from these observatories eventually led to the discovery that neutrinos have a very small ] and can indeed oscillate.<ref name="Schlattl">{{cite journal
|last=Schlattl
|first=H.
|year=2001
|title=Three-flavor oscillation solutions for the solar neutrino problem
|journal=Physical Review D
|volume=64
|issue=1}}</ref>. Moreover, the Sudbury Neutrino Observatory was able to detect all three types of neutrinos directly, and found that the Sun's ''total'' neutrino emission rate agreed with the Standard Solar Model, although only one-third of the neutrinos seen at Earth were of the electron type.


On April 28, 2021, NASA's ] encountered the specific magnetic and particle conditions at 18.8 solar radii that indicated that it penetrated the ], the boundary separating the corona from the solar wind, defined as where the coronal plasma's Alfvén speed and the large-scale solar wind speed are equal.<ref name="touching">{{cite web |last=Hatfield |first=Miles |title=NASA Enters the Solar Atmosphere for the First Time |url=https://www.nasa.gov/feature/goddard/2021/nasa-enters-the-solar-atmosphere-for-the-first-time-bringing-new-discoveries |website=NASA |date=13 December 2021 |access-date=30 July 2022 |archive-date=27 December 2021 |archive-url=https://web.archive.org/web/20211227093247/https://www.nasa.gov/feature/goddard/2021/nasa-enters-the-solar-atmosphere-for-the-first-time-bringing-new-discoveries/ |url-status=live }}{{PD-notice}}</ref><ref name=animation>{{cite web |title=GMS: Animation: NASA's Parker Solar Probe Enters Solar Atmosphere |url=https://svs.gsfc.nasa.gov/14036 |website=svs.gsfc.nasa.gov |access-date=30 July 2022 |date=14 December 2021 |archive-date=4 October 2022 |archive-url=https://web.archive.org/web/20221004004943/https://svs.gsfc.nasa.gov/14036 |url-status=live }}</ref> During the flyby, Parker Solar Probe passed into and out of the corona several times. This proved the predictions that the Alfvén critical surface is not shaped like a smooth ball, but has spikes and valleys that wrinkle its surface.<ref name="touching" />
===Coronal heating problem===
The optical surface of the Sun (the ]) is known to have a temperature of approximately 6,000 ]. Above it lies the solar corona at a temperature of 1,000,000&nbsp;K. The high temperature of the corona shows that it is heated by something other than direct heat ] from the photosphere.


]]]
It is thought that the energy necessary to heat the corona is provided by turbulent motion in the convection zone below the photosphere, and two main mechanisms have been proposed to explain coronal heating. The first is ] heating, in which sound, gravitational and magnetohydrodynamic waves are produced by turbulence in the convection zone. These waves travel upward and dissipate in the corona, depositing their energy in the ambient gas in the form of heat. The other is ] heating, in which magnetic energy is continuously built up by photospheric motion and released through ] in the form of large ]s and myriad similar but smaller events.<ref name="Alfven">{{cite journal
|last=Alfvén
|first=H.
|year=1947
|title=Magneto-hydrodynamic waves, and the heating of the solar corona
|journal=Monthly Notices of the Royal Astronomical Society
|volume=107
|pages=211}}</ref>


== Solar radiation ==
Currently, it is unclear whether waves are an efficient heating mechanism. All waves except Alfven waves have been found to dissipate or refract before reaching the corona.<ref name="Sturrock">{{cite journal
{{Main|Sunlight|Solar irradiance}}
|last=Sturrock
]
|first=P. A.
The Sun emits light across the ], so its color is ], with a ] color-space index near (0.3, 0.3), when viewed from space or when the Sun is high in the sky. The Solar radiance per wavelength peaks in the green portion of the spectrum when viewed from space.<ref>{{cite news |title=What Color is the Sun? |work=Universe Today |url=http://www.universetoday.com/18689/color-of-the-sun/ |url-status=live |access-date=23 May 2016 |archive-url=https://web.archive.org/web/20160525215525/http://www.universetoday.com/18689/color-of-the-sun/ |archive-date=25 May 2016}}</ref><ref>{{cite web |title=What Color is the Sun? |url=http://solar-center.stanford.edu/SID/activities/GreenSun.html |url-status=live |archive-url=https://web.archive.org/web/20171030154449/http://solar-center.stanford.edu/SID/activities/GreenSun.html |archive-date=30 October 2017 |access-date=23 May 2016 |publisher=] Solar Center}}</ref> When the Sun is very low in the sky, ] renders the Sun yellow, red, orange, or magenta, and in rare occasions even ]. Some cultures mentally picture the Sun as yellow and some even red; the cultural reasons for this are debated.<ref name="yellow sun paradox">{{Cite journal |last=Wilk |first=S. R. |date=2009 |title=The Yellow Sun Paradox |url=http://www.osa-opn.org/Content/ViewFile.aspx?id=11147 |url-status=dead |journal=] |pages=12–13 |archive-url=https://web.archive.org/web/20120618183229/http://www.osa-opn.org/Content/ViewFile.aspx?id=11147 |archive-date=18 June 2012}}</ref> The Sun is classed as a ''G2'' star,<ref name="Phillips1995-47" /> meaning it is a ], with ''2'' indicating its ] is in the second range of the G class.
|coauthors=Uchida, Y.
|year=1981
|url=http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1981ApJ...246..331S&amp;data_type=PDF_HIGH&amp;type=PRINTER&amp;filetype=.pdf
|title=Coronal heating by stochastic magnetic pumping
|journal=Astrophysical Journal
|volume=246
|pages=331}}</ref> In addition, Alfvén waves do not easily dissipate in the corona. Current research focus has therefore shifted towards flare heating mechanisms. One possible candidate to explain coronal heating is continuous flaring at small scales,<ref name="Parker2">{{cite journal
|last=Parker
|first=E. N.
|year=1988
|url=http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1988ApJ...330..474P&amp;data_type=PDF_HIGH&amp;type=PRINTER&amp;filetype=.pdf
|title=Nanoflares and the solar X-ray corona
|journal=Astrophysical Journal
|volume=330
|pages=474}}</ref> but this remains an open topic of investigation.


The ] 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 {{val|1368|u=W/m2|fmt=commas}} (watts per square meter) at a distance of one ] (AU) from the Sun (that is, at or near Earth's orbit).<ref name="TSI">{{cite web |title=Construction of a Composite Total Solar Irradiance (TSI) Time Series from 1978 to present |url=http://www.pmodwrc.ch/pmod.php?topic=tsi/composite/SolarConstant |date=24 May 2006 |website=pmodwrc |url-status=dead |archive-url=https://web.archive.org/web/20110801183920/http://www.pmodwrc.ch/pmod.php?topic=tsi%2Fcomposite%2FSolarConstant |archive-date=1 August 2011 |access-date=5 October 2005}}</ref> Sunlight on the surface of Earth is ] by ], so that less power arrives at the surface (closer to {{val|1000|u=W/m2|fmt=commas}}) in clear conditions when the Sun is near the ].<ref name="El-Sharkawi2005">{{Cite book |last=El-Sharkawi |first=Mohamed A. |title=Electric energy |date=2005 |publisher=CRC Press |isbn=978-0-8493-3078-0 |url=https://books.google.com/books?id=UokcachsYcYC&pg=PA87 |pages=87–88}}</ref> Sunlight at the top of Earth's atmosphere is composed (by total energy) of about 50% infrared light, 40% visible light, and 10% ultraviolet light.<ref name="Solar radiation">{{cite encyclopedia |entry=Radiation (Solar) |encyclopedia=Encyclopedia of Atmospheric Sciences |year=2003 |last=Fu |first=Qiang |title=Radiation (SOLAR) |editor-last1=Curry |editor-first1=Judith A. |editor-last2=Pyle |editor-first2=John A. |publisher=Elsevier |pages=1859–1863 |doi=10.1016/B0-12-227090-8/00334-1 |isbn=978-0-12-227090-1 |url=http://curry.eas.gatech.edu/Courses/6140/ency/Chapter3/Ency_Atmos/Radiation_Solar.pdf |url-status=dead |archive-url=https://web.archive.org/web/20121101070344/http://curry.eas.gatech.edu/Courses/6140/ency/Chapter3/Ency_Atmos/Radiation_Solar.pdf |archive-date=1 November 2012 |access-date=29 December 2012}}</ref> The atmosphere filters out over 70% of solar ultraviolet, especially at the shorter wavelengths.<ref>{{cite web |title=Reference Solar Spectral Irradiance: Air Mass 1.5 |url=http://rredc.nrel.gov/solar/spectra/am1.5/ |website=NREL |url-status=live |archive-url=https://web.archive.org/web/20190512190812/https://rredc.nrel.gov/solar//spectra/am1.5/ |archive-date=12 May 2019 |access-date=12 November 2009}}</ref> Solar ] ionizes Earth's dayside upper atmosphere, creating the electrically conducting ].<ref name="Phillips1995">{{Cite book |last=Phillips |first=K. J. H. |title=Guide to the Sun |url=https://books.google.com/books?id=idwBChjVP0gC&pg=PA14 |date=1995 |publisher=] |isbn=978-0-521-39788-9 |pages=14–15, 34–38}}</ref>
===Ultraviolet rays===
Simply put, ] (also known as ] or ]) is a form of energy traveling through space. Some of the most frequently recognized types of energy are heat and light. These, along with others, can be classified as a phenomenon known as electromagnetic radiation. Other types of ] are gamma rays, X-rays, visible light, infrared rays, and radio waves. The progression of ] through ] can be visualized in different ways. Some experiments suggest that these rays travel in the form of waves. A physicist can actually measure the length of those waves (simply called their wavelength). It turns out that a smaller ] means more ]. At other times, it is more plausible to describe ] as being contained and traveling in little packets, called ].


] light from the Sun has ] properties and can be used to sanitize tools and water. This radiation causes ], and has other biological effects such as the production of ] and ]. It is the main cause of ]. Ultraviolet light is strongly attenuated by Earth's ], so that the amount of UV varies greatly with ] and has been partially responsible for many biological adaptations, including variations in ].<ref>{{Cite journal |last=Barsh |first=G. S. |date=2003 |title=What Controls Variation in Human Skin Color? |journal=] |volume=1 |issue=1 |page=e7 |doi=10.1371/journal.pbio.0000027 |pmc=212702 |pmid=14551921 |doi-access=free }}</ref>
The distinguishing factor among the different types of ] is their energy content. ] is more energetic than visible ] and therefore has a shorter ]. To be more specific: Ultraviolet rays have a wavelength between approximately 100 nanometers and 400 nanometers whereas visible radiation includes wavelengths between 400 and 780 nanometers.


High-energy ] ]s initially released with fusion reactions in the core are almost immediately absorbed by the solar plasma of the radiative zone, usually after traveling only a few millimeters. Re-emission happens in a random direction and usually at slightly lower energy. With this sequence of emissions and absorptions, it takes a long time for radiation to reach the Sun's surface. Estimates of the photon travel time range between 10,000 and 170,000&nbsp;years.<ref name="NASA">{{cite web |date=2007 |title=Ancient sunlight |url=http://sunearthday.nasa.gov/2007/locations/ttt_sunlight.php |url-status=dead |archive-url=https://web.archive.org/web/20090515085541/http://sunearthday.nasa.gov/2007/locations/ttt_sunlight.php |archive-date=15 May 2009 |access-date=24 June 2009 |website=Technology Through Time |publisher=NASA |issue=50}}</ref> In contrast, it takes only 2.3&nbsp;seconds for ]s, which account for about 2% of the total energy production of the Sun, to reach the surface. Because energy transport in the Sun is a process that involves photons in ] equilibrium with ], the time scale of energy transport in the Sun is longer, on the order of 30,000,000&nbsp;years. This is the time it would take the Sun to return to a stable state if the rate of energy generation in its core were suddenly changed.<ref>{{Cite journal |last=Stix |first=M. |date=2003 |title=On the time scale of energy transport in the sun |journal=] |volume=212 |issue=1 |pages=3–6 |bibcode=2003SoPh..212....3S |doi=10.1023/A:1022952621810 |s2cid=118656812}}</ref>
The Sun emits ultraviolet radiation in the UVA, UVB, and UVC bands, but because of absorption in the atmosphere's ozone layer, 99% of the ultraviolet radiation that reaches the Earth's surface is UVA. (Some of the UVC light is responsible for the generation of the ozone.)


]s are released by fusion reactions in the core, but, unlike photons, they rarely interact with matter, so almost all are able to escape the Sun immediately. However, measurements of the number of these neutrinos produced in the Sun are ] by a factor of 3. In 2001, the discovery of ] resolved the discrepancy: the Sun emits the number of electron neutrinos predicted by the theory, but neutrino detectors were missing {{frac|2|3}} of them because the neutrinos had changed ] by the time they were detected.<ref name="Schlattl">{{Cite journal |last=Schlattl |first=H. |date=2001 |title=Three-flavor oscillation solutions for the solar neutrino problem |journal=] |volume=64 |issue=1 |page=013009 |arxiv=hep-ph/0102063 |bibcode=2001PhRvD..64a3009S |doi=10.1103/PhysRevD.64.013009 |s2cid=117848623}}</ref>
Ordinary glass is partially transparent to UVA but is opaque to shorter wavelengths while Silica or quartz glass, depending on quality, can be transparent even to vacuum UV wavelengths. Ordinary window glass passes about 90% of the light above 350 nm, but blocks over 90% of the light below 300 nm.


== Magnetic activity ==
The onset of vacuum UV, 200 nm, is defined by the fact that ordinary air is opaque below this wavelength. This opacity is due to the strong absorption of light of these wavelengths by oxygen in the air. Pure nitrogen (less than about 10 ppm oxygen) is transparent to ] in the range of about 150–200 nm. This has wide practical significance now that semiconductor manufacturing processes are using wavelengths shorter than 200 nm. By working in oxygen-free gas, the equipment does not have to be built to withstand the pressure differences required to work in a vacuum. Some other scientific instruments, such as circular dichroism spectrometers, are also commonly nitrogen purged and operate in this spectral region.


The Sun has a ] that varies across its surface. Its polar field is {{convert|1|-|2|G|sigfig=1|lk=on}}, whereas the field is typically {{convert|3000|G|sigfig=1}} in features on the Sun called ]s and {{convert|10|-|100|G|sigfig=1}} in ]s.<ref name="nssdc" /> The magnetic field varies in time and location. The quasi-periodic 11-year ] is the most prominent variation in which the number and size of sunspots waxes and wanes.<ref name="doi10.1146/annurev-astro-081913-040012">{{Cite journal |doi=10.1146/annurev-astro-081913-040012 |title=Solar Dynamo Theory |journal=Annual Review of Astronomy and Astrophysics |volume=52 |pages=251–290 |year=2014 |last1=Charbonneau |first1=P. |bibcode=2014ARA&A..52..251C|s2cid=17829477 |doi-access=free }}</ref><ref name="Zirker2002-119">{{Cite book |last=Zirker |first=J. B. |date=2002 |title=Journey from the Center of the Sun |pages= |publisher=] |isbn=978-0-691-05781-1 |url=https://archive.org/details/journeyfromcente0000zirk/page/119 }}</ref><ref name="Lang">{{Cite book |last=Lang |first=Kenneth R. |date=2008 |title=The Sun from Space |page=75 |publisher=] |isbn=978-3-540-76952-1}}</ref>
Extreme UV is characterized by a transition in the physics of interaction with matter: wavelengths longer than about 30 nm interact mainly with the chemical valence ] of matter, while wavelengths shorter than that interact mainly with inner shell electrons and nuclei. The long end of the EUV/XUV spectrum is set by a prominent He+ spectral line at 30.4nm. XUV is strongly absorbed by most known materials, but it is possible to synthesize multilayer optics that reflect up to about 50% of XUV radiation at normal incidence. This technology has been used to make ] for solar imaging; it was pioneered by the NIXT and MSSTA sounding rockets in the 1990s; (current examples are SOHO/EIT and TRACE) and for ] (printing of traces and devices on microchips).


The solar magnetic field extends well beyond the Sun itself. The electrically conducting solar wind plasma carries the Sun's magnetic field into space, forming what is called the ].<ref name="Russell2001" /> In an approximation known as ideal ], plasma particles only move along magnetic field lines. As a result, the outward-flowing solar wind stretches the interplanetary magnetic field outward, forcing it into a roughly radial structure. For a simple dipolar solar magnetic field, with opposite hemispherical polarities on either side of the solar magnetic equator, a thin ] is formed in the solar wind. At great distances, the rotation of the Sun twists the dipolar magnetic field and corresponding current sheet into an ] structure called the ''Parker spiral''.<ref name="Russell2001" />
===Faint young Sun problem===
{{main|Faint young Sun paradox}}


=== Sunspot ===
Theoretical models of the Sun's development suggest that 3.8 to 2.5 billion years ago, during the ], the Sun was only about 75% as bright as it is today. Such a weak star would not have been able to sustain liquid water on the Earth's surface, and thus life should not have been able to develop. However, the geological record demonstrates that the Earth has remained at a fairly constant temperature throughout its history, and in fact that the young Earth was somewhat warmer than it is today. The general consensus among scientists is that the young Earth's atmosphere contained much larger quantities of ]es (such as ] and/or ]) than are present today, which trapped enough heat to compensate for the lesser amount of solar energy reaching the planet.<ref name="Kasting">{{cite journal
{{Main|Sunspot}}
|last=Kasting
]
|first=J. F.
|coauthors=Ackerman, T. P.
|year=1986
|title=Climatic Consequences of Very High Carbon Dioxide Levels in the Earth’s Early Atmosphere
|journal=Science
|volume=234
|pages=1383-1385}}</ref>


Sunspots are visible as dark patches on the Sun's photosphere and correspond to concentrations of magnetic field where convective transport of heat is inhibited from the solar interior to the surface. As a result, sunspots are slightly cooler than the surrounding photosphere, so they appear dark. At a typical ], few sunspots are visible, and occasionally none can be seen at all. Those that do appear are at high solar latitudes. As the solar cycle progresses toward its ], sunspots tend to form closer to the solar equator, a phenomenon known as '']''. The largest sunspots can be tens of thousands of kilometers across.<ref name="Sunspot2001">{{cite web |date=30 March 2001 |title=The Largest Sunspot in Ten Years |url=http://www.gsfc.nasa.gov/gsfc/spacesci/solarexp/sunspot.htm |publisher=] |access-date=10 July 2009 |url-status=dead |archive-url=https://web.archive.org/web/20070823050403/http://www.gsfc.nasa.gov/gsfc/spacesci/solarexp/sunspot.htm |archive-date=23 August 2007}}</ref>
==Magnetic field==
] extends to the outer reaches of the Solar System, and results from the influence of the Sun's rotating magnetic field on the ] in the ] ]]


An 11-year sunspot cycle is half of a 22-year ]–Leighton ] cycle, which corresponds to an oscillatory exchange of energy between ] solar magnetic fields. At solar-cycle maximum, the external poloidal dipolar magnetic field is near its dynamo-cycle minimum strength; but an internal toroidal quadrupolar field, generated through differential rotation within the tachocline, is near its maximum strength. At this point in the dynamo cycle, buoyant upwelling within the convective zone forces emergence of the toroidal magnetic field through the photosphere, giving rise to pairs of sunspots, roughly aligned east–west and having footprints with opposite magnetic polarities. The magnetic polarity of sunspot pairs alternates every solar cycle, a phenomenon described by ].<ref>{{Cite journal |last1=Hale |first1=G. E. |last2=Ellerman |first2=F. |last3=Nicholson |first3=S. B. |last4=Joy |first4=A. H. |title=The Magnetic Polarity of Sun-Spots |journal=The Astrophysical Journal |volume=49 |page=153 |year=1919 |doi=10.1086/142452 |bibcode=1919ApJ....49..153H|doi-access=free }}</ref><ref name="solarcycle">{{cite web |date=4 January 2008 |title=NASA Satellites Capture Start of New Solar Cycle |publisher=] |url=http://www.physorg.com/news119271347.html |access-date=10 July 2009 |archive-date=6 April 2008 |archive-url=https://web.archive.org/web/20080406132839/http://www.physorg.com/news119271347.html |url-status=live }}</ref>
All ] in the Sun is in the form of ] and ] because of its high temperatures. This makes it possible for the Sun to rotate faster at its equator (about 25 days) than it does at higher latitudes (about 35 days near its poles). The ] of the Sun's latitudes causes its ] lines to become twisted together over time, causing magnetic field loops to erupt from the Sun's surface and trigger the formation of the Sun's dramatic ]s and ]s (see ]). This twisting action gives rise to the ] and an 11-year ] of magnetic activity as the Sun's magnetic field reverses itself about every 11 years.


During the solar cycle's declining phase, energy shifts from the internal toroidal magnetic field to the external poloidal field, and sunspots diminish in number and size. At solar-cycle minimum, the toroidal field is, correspondingly, at minimum strength, sunspots are relatively rare, and the poloidal field is at its maximum strength. With the rise of the next 11-year sunspot cycle, differential rotation shifts magnetic energy back from the poloidal to the toroidal field, but with a polarity that is opposite to the previous cycle. The process carries on continuously, and in an idealized, simplified scenario, each 11-year sunspot cycle corresponds to a change, then, in the overall polarity of the Sun's large-scale magnetic field.<ref>{{Cite news |date=16 February 2001 |title=Sun flips magnetic field |url=http://edition.cnn.com/2001/TECH/space/02/16/sun.flips/ |work=] |access-date=11 July 2009 |archive-date=21 January 2015 |archive-url=https://web.archive.org/web/20150121063331/http://edition.cnn.com/2001/TECH/space/02/16/sun.flips/ |url-status=live }}</ref><ref>{{cite web |last=Phillips |first=T. |date=15 February 2001 |title=The Sun Does a Flip |url=https://science.nasa.gov/headlines/y2001/ast15feb_1.htm |publisher=NASA |access-date=11 July 2009 |url-status=dead |archive-url=https://web.archive.org/web/20090512121817/https://science.nasa.gov/headlines/y2001/ast15feb_1.htm |archive-date=12 May 2009 }}</ref>
The influence of the Sun's ] on the plasma in the ] creates the ], which separates regions with magnetic fields pointing in different directions. The plasma in the interplanetary medium is also responsible for the strength of the Sun's magnetic field at the orbit of the Earth. If space were a vacuum, then the Sun's 10<sup>-4</sup> ] magnetic dipole field would reduce with the cube of the distance to about 10<sup>-11</sup> tesla. But satellite observations show that it is about 100 times greater at around 10<sup>-9</sup> tesla. ] (MHD) theory predicts that the motion of a conducting fluid (e.g., the interplanetary medium) in a magnetic field, induces electric currents which in turn generates magnetic fields, and in this respect it behaves like an ].


=== Solar activity ===
==History of solar observation==
{{Main||Solar cycle}}
===Early understanding of the Sun===
]
] pulled by a horse is a sculpture believed to be illustrating an important part of ] mythology.]]


The Sun's magnetic field leads to many effects that are collectively called ]. ] and ] tend to occur at sunspot groups. Slowly changing high-speed streams of solar wind are emitted from ] at the photospheric surface. Both coronal mass ejections and high-speed streams of solar wind carry plasma and the interplanetary magnetic field outward into the Solar System.<ref name=Zirker2002>{{Cite book |last=Zirker |first=J. B. |date=2002 |title=Journey from the Center of the Sun |pages= |publisher=] |isbn=978-0-691-05781-1 |url=https://archive.org/details/journeyfromcente0000zirk/page/120 }}</ref> The effects of solar activity on Earth include ] at moderate to high latitudes and the disruption of radio communications and ]. Solar activity is thought to have played a large role in the ].<ref>{{cite journal |last1=Nandy |first1=Dibyendu |last2=Martens |first2=Petrus C. H. |last3=Obridko |first3=Vladimir |last4=Dash |first4=Soumyaranjan |last5=Georgieva |first5=Katya |title=Solar evolution and extrema: current state of understanding of long-term solar variability and its planetary impacts |journal=Progress in Earth and Planetary Science |date=5 July 2021 |volume=8 |issue=1 |pages=40 |doi=10.1186/s40645-021-00430-x |doi-access=free |bibcode=2021PEPS....8...40N |issn=2197-4284}}</ref>
Humanity's most fundamental understanding of the Sun is as the luminous disk in the ], whose presence above the ] creates day and whose absence causes night. In many prehistoric and ancient cultures, the Sun was thought to be a ] or other ] phenomenon, and ] of the Sun was central to civilizations such as the ] of ] and the ]s of what is now ]. Many ancient monuments were constructed with solar phenomena in mind; for example, stone ]s accurately mark the ] (some of the most prominent megaliths are located in ], ], and at ] in ]); the pyramid of ] at ] in Mexico is designed to cast shadows in the shape of serpents climbing the pyramid at the vernal and autumn ]es. With respect to the ]s, the Sun appears from Earth to revolve once a year along the ] through the ], and so the Sun was considered by Greek astronomers to be one of the seven ]s (Greek ''planetes'', "wanderer"), after which the seven days of the ] are named in some languages.


Long-term secular change in sunspot number is thought, by some scientists, to be correlated with long-term change in solar irradiance,<ref>{{cite journal |last1=Willson |first1=R. C. |last2=Hudson |first2=H. S. |date=1991 |title=The Sun's luminosity over a complete solar cycle |journal=] |volume=351 |issue=6321 |pages=42–44 |doi=10.1038/351042a0 |bibcode=1991Natur.351...42W|s2cid=4273483 }}</ref> which, in turn, might influence Earth's long-term climate.<ref>{{cite journal |author-link=John A. Eddy |last=Eddy |first=John A. |title=The Maunder Minimum |journal=] |volume=192 |issue=4245 |pages=1189–1202 |date=June 1976 |pmid=17771739 |doi=10.1126/science.192.4245.1189 |jstor=1742583 |bibcode=1976Sci...192.1189E|s2cid=33896851 }}</ref> The solar cycle influences ] conditions, including those surrounding Earth. For example, in the 17th century, the solar cycle appeared to have stopped entirely for several decades; few sunspots were observed during a period known as the ]. This coincided in time with the era of the ], when Europe experienced unusually cold temperatures.<ref name="Lean">{{Cite journal |last1=Lean |first1=J. |author-link=Judith Lean |last2=Skumanich |first2=A. |last3=White |first3=O. |date=1992 |title=Estimating the Sun's radiative output during the Maunder Minimum |journal=] |volume=19 |issue=15 |pages=1591–1594 |doi=10.1029/92GL01578 |bibcode=1992GeoRL..19.1591L |url=https://zenodo.org/record/1231321 |access-date=16 December 2019 |archive-date=11 May 2020 |archive-url=https://web.archive.org/web/20200511052658/https://zenodo.org/record/1231321 |url-status=live }}</ref> Earlier extended minima have been discovered through analysis of ]s and appear to have coincided with lower-than-average global temperatures.<ref>{{Cite book |last1=Mackay |first1=R. M. |last2=Khalil |first2=M. A. K. |chapter=Greenhouse gases and global warming |chapter-url=https://books.google.com/books?id=tQBS3bAX8fUC&q=solar+minimum+dendochronology&pg=PA1 |editor-last=Singh | editor-first=S. N. |date=2000 |title=Trace Gas Emissions and Plants |pages=1–28 |publisher=] |isbn=978-0-7923-6545-7 |access-date=3 November 2020 |archive-date=17 April 2021 |archive-url=https://web.archive.org/web/20210417054703/https://books.google.com/books?id=tQBS3bAX8fUC&q=solar+minimum+dendochronology&pg=PA1 |url-status=live }}</ref>
===Development of modern scientific understanding===
] ]. The black circle is the size of the orbit of Mars. ] is also included in the picture for comparison.]]
] ] (Sun can only be seen when image is clicked on twice)]]
One of the first people in the Western world to offer a scientific explanation for the Sun was the ] ] ], who reasoned that it was a giant flaming ball of metal even larger than the ], and not the ] of ]. For teaching this ], he was imprisoned by the authorities and ] (though later released through the intervention of ]). ] might have been the first person to have accurately calculated the distance from the Earth to the Sun, in the 3rd century BCE, as 149 million kilometers, roughly the same as the modern accepted figure.


=== Coronal heating ===
Another scientist to challenge the accepted view was ], who in the 16th century developed the theory that the Earth orbited the Sun, rather than the other way around. In the early 17th century, ] pioneered ] observations of the Sun, making some of the first known observations of sunspots and positing that they were on the surface of the Sun rather than small objects passing between the Earth and the Sun.<ref>{{cite web
{{Main|Stellar corona}}
|url=http://www.bbc.co.uk/history/historic_figures/galilei_galileo.shtml
{{unsolved|astronomy|Why is the Sun's corona so much hotter than the Sun's surface?}}
|title=Galileo Galilei (1564 - 1642)
|publisher=BBC
|accessdate=2006-03-22}}</ref> ] observed the Sun's light using a ], and showed that it was made up of light of many colors,<ref>{{cite web
|url=http://www.bbc.co.uk/history/historic_figures/newton_isaac.shtml
|title=Sir Isaac Newton (1643 - 1727)
|publisher=BBC
|accessdate=2006-03-22}}</ref> while in 1800 ] discovered ] radiation beyond the red part of the solar spectrum.<ref>{{cite web
|url=http://coolcosmos.ipac.caltech.edu/cosmic_classroom/classroom_activities/herschel_bio.html
|title=Herschel Discovers Infrared Light
|publisher=Cool Cosmos
|accessdate=2006-03-22}}</ref> The 1800s saw spectroscopic studies of the Sun advance, and ] made the first observations of ] in the spectrum, the strongest of which are still often referred to as Fraunhofer lines.


The temperature of the photosphere is approximately 6,000&nbsp;K, whereas the temperature of the corona reaches {{val|1000000|-|2000000|u=K|fmt=commas}}.<ref name="Erdelyi2007" /> The high temperature of the corona shows that it is heated by something other than direct ] from the photosphere.<ref name="Russell2001" />
In the early years of the modern scientific era, the source of the Sun's energy was a significant puzzle. ] suggested that the Sun was a gradually cooling liquid body that was radiating an internal store of heat.<ref>{{cite journal
|last=Thomson
|first=Sir William
|title=On the Age of the Sun’s Heat
|journal=Macmillan's Magazine
|year=1862
|volume=5
|pages=288-293
|url=http://zapatopi.net/kelvin/papers/on_the_age_of_the_suns_heat.html}}</ref> Kelvin and ] then proposed the ] to explain the energy output. Unfortunately the resulting age estimate was only 20 million years,
well short of the time span of several billion years suggested by geology. In 1890 ], the discoverer of helium in the solar spectrum, proposed a meteoritic hypothesis for the formation and evolution of the sun.<ref>{{cite book
|last=Lockyer
|first=Joseph Norman
|title=The meteoritic hypothesis; a statement of the results of a spectroscopic inquiry into the origin of cosmical systems
|publisher=Macmillan and Co.
|location=London and New York
|year=1890
|url=http://adsabs.harvard.edu/abs/1890QB981.L78......}}</ref> Another proposal was that the Sun extracted its energy from friction of its gas masses.{{Fact}}


It is thought that the energy necessary to heat the corona is provided by turbulent motion in the convection zone below the photosphere, and two main mechanisms have been proposed to explain coronal heating.<ref name="Erdelyi2007" /> The first is wave heating, in which sound, gravitational or magnetohydrodynamic waves are produced by turbulence in the convection zone.<ref name="Erdelyi2007" /> These waves travel upward and dissipate in the corona, depositing their energy in the ambient matter in the form of heat.<ref name="Alfven">{{Cite journal |last=Alfvén |first=H. |date=1947 |title=Magneto-hydrodynamic waves, and the heating of the solar corona |journal=] |volume=107 |issue=2 |pages=211–219 |bibcode=1947MNRAS.107..211A |doi=10.1093/mnras/107.2.211 |doi-access=free}}</ref> The other is magnetic heating, in which magnetic energy is continuously built up by photospheric motion and released through ] in the form of large solar flares and myriad similar but smaller events—].<ref name="Parker2">{{Cite journal |last=Parker |first=E. N. |date=1988 |title=Nanoflares and the solar X-ray corona |journal=] |volume=330 |issue=1 |page=474 |bibcode=1988ApJ...330..474P |doi=10.1086/166485}}</ref>
It would be 1904 before a potential solution was offered. ] suggested that the energy could be maintained by an internal source of heat, and suggested ] as the source.<ref>{{cite web
|last=Darden
|first=Lindley
|year=1998
|title=The Nature of Scientific Inquiry
|journal=Macmillan's Magazine
|url=http://www.philosophy.umd.edu/Faculty/LDarden/sciinq/}}</ref> However it would be ] who would provide the essential clue to the source of a Sun's energy with his mass-energy relation ].
In 1920 Sir ] proposed that the pressures and temperatures at the core of the Sun could produce a nuclear fusion reaction that merged hydrogen into helium, resulting in a production of energy from the net change in mass.<ref>{{cite web
|date=2005-06-15
|title=Studying the stars, testing relativity: Sir Arthur Eddington
|journal=ESA Space Science
|url=http://www.esa.int/esaSC/SEMDYPXO4HD_index_0.html}}</ref> This theoretical concept was developed
in the 1930s by the astrophysicists ] and ]. Hans Bethe calculated the details of the two main energy-producing nuclear reactions that power the Sun.<ref name="Bethe">{{cite journal
|last=Bethe
|first=H.
|year=1938
|title=On the Formation of Deuterons by Proton Combination
|journal=Physical Review
|volume=54
|pages=862-862}}</ref><ref name="Bethe2">{{cite journal
|last=Bethe
|first=H.
|year=1939
|title=Energy Production in Stars
|journal=Physical Review
|volume=55
|pages=434-456}}</ref>


Currently, it is unclear whether waves are an efficient heating mechanism. All waves except Alfvén waves have been found to dissipate or refract before reaching the corona.<ref name="Sturrock">{{Cite journal |last1=Sturrock |first1=P. A. |last2=Uchida |first2=Y. | year=1981 |title=Coronal heating by stochastic magnetic pumping |journal=] |volume=246 |issue=1 |page=331 |bibcode=1981ApJ...246..331S |doi=10.1086/158926 |hdl-access=free |hdl=2060/19800019786}}</ref> In addition, Alfvén waves do not easily dissipate in the corona. Current research focus has therefore shifted towards flare heating mechanisms.<ref name="Erdelyi2007" />
Finally, in 1957, a paper titled ''Synthesis of the Elements in Stars''<ref>{{cite journal
|author=E. Margaret Burbidge; G. R. Burbidge; William A. Fowler; F. Hoyle
|title=Synthesis of the Elements in Stars
|journal=Reviews of Modern Physics
|year=1957
|volume=29
|issue=4
|pages=547-650
|url=http://adsabs.harvard.edu/abs/1957RvMP...29..547B}}</ref> was published that demonstrated convincingly that most of the elements in the universe had been created by nuclear reactions inside stars like the Sun.


== Life phases ==
===Solar space missions===
{{Main|Formation and evolution of the Solar System|Stellar evolution}}
]" in sequence as recorded in November 2000 by four instruments onboard the ] spacecraft.]]
] at left to ] stage at right|alt=See caption]]
The Sun today is roughly halfway through the main-sequence portion of its life. It has not changed dramatically in over four billion<ref group=lower-alpha name=short /> years and will remain fairly stable for about five billion more. However, after hydrogen fusion in its core has stopped, the Sun will undergo dramatic changes, both internally and externally.


=== Formation ===
The first satellites designed to observe the Sun were ]'s ]s 5, 6, 7, 8 and 9, which were launched between 1959 and 1968. These probes orbited the Sun at a distance similar to that of the Earth's orbit, and made the first detailed measurements of the solar wind and the solar magnetic field. Pioneer 9 operated for a particularly long period of time, transmitting data until 1987.<ref>{{cite web
{{further|Formation and evolution of the Solar System}}
|url=http://www.astronautix.com/craft/pio6789e.htm
The Sun formed about 4.6&nbsp;billion years ago from the collapse of part of a giant ] that consisted mostly of hydrogen and helium and that probably gave birth to many other stars.<!-- We would say 4.57, but there may be uncertainty; for example, https://arxiv.org/pdf/1507.05847.pdf seems to suggest 4.587 rather than 4.567 --><ref name=Zirker2002-7>{{Cite book |last=Zirker |first=Jack B. |title=Journey from the Center of the Sun |date=2002 |publisher=] |isbn=978-0-691-05781-1 |pages=7–8}}</ref> This age is estimated using ] of ] and through ].<ref name="Bonanno" /> The result is consistent with the ] of the oldest Solar System material, at 4.567&nbsp;billion years ago.<ref>{{Cite journal |last1=Amelin |first1=Y. |last2=Krot |first2=A. |last3=Hutcheon |first3=I. |last4=Ulyanov |first4=A. |title=Lead isotopic ages of chondrules and calcium-aluminum-rich inclusions |journal=] |volume=297 |issue=5587 |pages=1678–1683 |date=2002 |doi=10.1126/science.1073950 |pmid=12215641|bibcode=2002Sci...297.1678A|s2cid=24923770 }}</ref><ref name="nature436">{{Cite journal |last1=Baker |first1=J. |last2=Bizzarro |first2=M. |last3=Wittig |first3=N. |last4=Connelly |first4=J. |last5=Haack |first5=H. |title=Early planetesimal melting from an age of 4.5662 Gyr for differentiated meteorites |journal=] |volume=436 |issue=7054 |pages=1127–1131 |date=2005 |pmid=16121173 |doi=10.1038/nature03882|bibcode=2005Natur.436.1127B|s2cid=4304613 }}</ref> Studies of ancient ]s reveal traces of stable daughter nuclei of short-lived isotopes, such as ], that form only in exploding, short-lived stars. This indicates that one or more ]e must have occurred near the location where the Sun formed. A ] from a nearby supernova would have triggered the formation of the Sun by compressing the matter within the molecular cloud and causing certain regions to collapse under their own gravity.<ref>{{Cite journal |last1=Williams |first1=J. |title=The astrophysical environment of the solar birthplace |journal=Contemporary Physics |volume=51 |issue=5 |pages=381–396 |year=2010 |doi=10.1080/00107511003764725 |bibcode=2010ConPh..51..381W |arxiv=1008.2973 |citeseerx=10.1.1.740.2876|s2cid=118354201 }}</ref> As one fragment of the cloud collapsed it also began to rotate due to ] and heat up with the increasing pressure.<ref>{{Cite web |last=Glozman |first=Igor |date=2022 |title=Formation of the Solar System |url=https://people.highline.edu/iglozman/classes/astronotes/solsys_form.htm |access-date=2022-01-16 |website=] |publication-place=Des Moines, WA |archive-date=26 March 2023 |archive-url=https://web.archive.org/web/20230326035535/https://people.highline.edu/iglozman/classes/astronotes/solsys_form.htm |url-status=live }}</ref> Much of the mass became concentrated in the center, whereas the rest flattened out into a disk that would become the planets and other Solar System bodies.<ref>{{cite journal |last1=D'Angelo |first1=G. |last2=Lubow |first2=S. H. |title=Three-dimensional Disk-Planet Torques in a Locally Isothermal Disk |journal=The Astrophysical Journal|date=2010|volume=724 |issue=1 |pages=730–747 |doi=10.1088/0004-637X/724/1/730 |arxiv=1009.4148 |bibcode=2010ApJ...724..730D |s2cid=119204765}}</ref><ref>{{cite book|last1=Lubow |first1=S. H. |last2=Ida |first2=S. |chapter=Planet Migration |bibcode=2010exop.book..347L |title=Exoplanets |publisher=University of Arizona Press |location=Tucson | editor-first=S. |editor-last=Seager |pages=347–371 |year=2011 |arxiv=1004.4137}}</ref> Gravity and pressure within the core of the cloud generated a lot of heat as it accumulated more matter from the surrounding disk, eventually triggering ].<ref>{{Cite web |last=Jones |first=Andrew Zimmerman |date=May 30, 2019 |title=How Stars Make All of the Elements |url=https://www.thoughtco.com/stellar-nucleosynthesis-2699311 |access-date=2023-01-16 |website=] |archive-date=11 July 2023 |archive-url=https://web.archive.org/web/20230711191648/https://www.thoughtco.com/stellar-nucleosynthesis-2699311 |url-status=live }}</ref>
|publisher=Encyclopedia Astronautica
|title=Pioneer 6-7-8-9-E
|accessdate=2006-03-22}}</ref>


The stars ] and ] share similarities with the Sun and are thus hypothesized to be its stellar siblings, formed in the same molecular cloud.<ref>{{cite web|url=http://www.natureworldnews.com/articles/6974/20140509/astronomers-find-suns-sibling-called-hd-162826.htm|title=Astronomers Find Sun's Sibling 'HD 162826'|date=May 9, 2014|publisher=Nature World News|access-date=2022-01-16|archive-date=3 March 2016|archive-url=https://web.archive.org/web/20160303235530/http://www.natureworldnews.com/articles/6974/20140509/astronomers-find-suns-sibling-called-hd-162826.htm|url-status=live}}</ref><ref>{{cite web |url=https://www.universetoday.com/140598/astronomers-find-one-of-the-suns-sibling-stars-born-from-the-same-solar-nebula-billion-of-years-ago/ |title=Astronomers Find One of the Sun's Sibling Stars. Born From the Same Solar Nebula Billions of Years Ago |first=Matt |last=Williams |date=2018-11-21 |website=] |access-date=2022-10-07 |archive-date=26 March 2023 |archive-url=https://web.archive.org/web/20230326035623/https://www.universetoday.com/140598/astronomers-find-one-of-the-suns-sibling-stars-born-from-the-same-solar-nebula-billion-of-years-ago/ |url-status=live }}</ref>
In the 1970s, ] and the ] ] provided scientists with significant new data on solar wind and the solar corona. The Helios 1 satellite was a joint ]-] probe that studied the solar wind from an orbit carrying the spacecraft inside ]'s orbit at ]. The Skylab space station, launched by NASA in 1973, included a solar ] module called the Apollo Telescope Mount that was operated by astronauts resident on the station. Skylab made the first time-resolved observations of the solar transition region and of ultraviolet emissions from the solar corona. Discoveries included the first observations of ]s, then called "coronal transients", and of ]s, now known to be intimately associated with the ].


=== Main sequence ===
In 1980, the ] was launched by ]. This spacecraft was designed to observe ]s, ]s and ] radiation from ]s during a time of high solar activity. Just a few months after launch, however, an electronics failure caused the probe to go into standby mode, and it spent the next three years in this inactive state. In 1984 ] ] mission STS-41C retrieved the satellite and repaired its electronics before re-releasing it into orbit. The Solar Maximum Mission subsequently acquired thousands of images of the solar corona before ] the Earth's atmosphere in June 1989.<ref>{{cite web
] is shown from the main sequence to the post-asymptotic-giant-branch stage.|300x300px|alt=See caption]]
|url=http://web.hao.ucar.edu/public/research/svosa/smm/smm_mission.html
The Sun is about halfway through its main-sequence stage, during which nuclear fusion reactions in its core fuse hydrogen into helium. Each second, more than four billion kilograms of matter are converted into energy within the Sun's core, producing neutrinos and ]. At this rate, the Sun has so far converted around 100 times the mass of Earth into energy, about 0.03% of the total mass of the Sun. The Sun will spend a total of approximately 10 to 11&nbsp;billion years as a main-sequence star before the ] phase of the Sun.<ref>{{Cite book |last1=Goldsmith |first1=D. |last2=Owen |first2=T. |title=The search for life in the universe |url=https://books.google.com/books?id=Q17NmHY6wloC&pg=PA96 |page=96 |publisher=University Science Books |year=2001 |isbn=978-1-891389-16-0 |access-date=22 August 2020 |archive-date=30 October 2020 |archive-url=https://web.archive.org/web/20201030203521/https://books.google.com/books?id=Q17NmHY6wloC&pg=PA96 |url-status=live }}</ref> At the 8 billion year mark, the Sun will be at its hottest point according to the ESA's '']'' space observatory mission in 2022.<ref>{{Cite web |date=2022-08-12 |title=ESA's Gaia Mission Sheds New Light on Past and Future of Our Sun |url=https://www.sci.news/astronomy/sun-future-11093.html |access-date=2022-08-15 |website=Sci.News: Breaking Science News |archive-date=4 April 2023 |archive-url=https://web.archive.org/web/20230404001136/https://www.sci.news/astronomy/sun-future-11093.html |url-status=live}}</ref>
|title=Solar Maximum Mission Overview
|first=Chris
|last=St. Cyr
|coauthors=Joan Burkepile
|accessdate=2006-03-22
|year=1998}}</ref>


The Sun is gradually becoming hotter in its core, hotter at the surface, larger in radius, and more luminous during its time on the main sequence: since the beginning of its main sequence life, it has expanded in radius by 15% and the surface has increased in temperature from {{Convert|5,620|K|F}} to {{Convert|5,772|K|F}}, resulting in a 48% increase in luminosity from 0.677 ] to its present-day 1.0 solar luminosity. This occurs because the helium atoms in the core have a higher mean ] than the ]s that were fused, resulting in less thermal pressure. The core is therefore shrinking, allowing the outer layers of the Sun to move closer to the center, releasing ]. According to the ], half of this released gravitational energy goes into heating, which leads to a gradual increase in the rate at which fusion occurs and thus an increase in the luminosity. This process speeds up as the core gradually becomes denser.<ref name="carroll_ostlie">{{cite book |last1=Carroll |first1=Bradley W. |title=An introduction to modern astrophysics |last2=Ostlie |first2=Dal A |date=2017 |publisher=Cambridge University Press |isbn=978-1-108-42216-1 |edition=Second |location=Cambridge, United Kingdom |pages=350, 447, 448, 457}}</ref> At present, it is increasing in brightness by about 1% every 100&nbsp;million years. It will take at least 1&nbsp;billion years from now to deplete liquid water from the Earth from such increase.<ref>{{cite web | first=Puneet | last=Kollipara | url=https://www.science.org/content/article/earth-wont-die-soon-thought | title=Earth Won't Die as Soon as Thought | work=Science | date=22 January 2014 | access-date=24 May 2015 | archive-date=12 November 2020 | archive-url=https://web.archive.org/web/20201112023013/https://www.sciencemag.org/news/2014/01/earth-wont-die-soon-thought | url-status=live }}</ref> After that, the Earth will cease to be able to support complex, multicellular life and the last remaining multicellular organisms on the planet will suffer a final, complete ].<ref name="Snyder-BeattieAndBonsall2022">{{cite journal |last1=Snyder-Beattie |first1=Andrew E. |last2=Bonsall |first2=Michael B. |date=30 March 2022 |title=Catastrophe risk can accelerate unlikely evolutionary transitions |journal=Proceedings of the Royal Society B |volume=289 |issue=1971 |doi=10.1098/rspb.2021.2711 |pmid=35350860 |pmc=8965398 }}</ref>
]'s ] (''Sunbeam'') satellite, launched in 1991, observed solar flares at X-ray wavelengths. Mission data allowed scientists to identify several different types of flares, and also demonstrated that the corona away from regions of peak activity was much more dynamic and active than had previously been supposed. Yohkoh observed an entire solar cycle but went into standby mode when an ] in 2001 caused it to lose its lock on the Sun. It was destroyed by atmospheric reentry in 2005.<ref>{{cite web
|url=http://www.jaxa.jp/press/2005/09/20050913_yohkoh_e.html
|title=Result of Re-entry of the Solar X-ray Observatory "Yohkoh" (SOLAR-A) to the Earth's Atmosphere
|year= 2005
|author=Japan Aerospace Exploration Agency
|accessdate=2006-03-22}}</ref>


=== After core hydrogen exhaustion ===
One of the most important solar missions to date has been the ], jointly built by the ] and ] and launched on ], ]. Originally a two-year mission, SOHO has now operated for over ten years (as of 2006). It has proved so useful that a follow-on mission, the ], is planned for launch in 2008. Situated at the ] between the Earth and the Sun (at which the gravitational pull from both is equal), SOHO has provided a constant view of the Sun at many wavelengths since its launch. In addition to its direct solar observation, SOHO has enabled the discovery of large numbers of comets, mostly very tiny ]s which incinerate as they pass the Sun.<ref>{{cite web
<!-- ] redirects to this section, please fix that if renaming this section. Thanks! -->
|url=http://ares.nrl.navy.mil/sungrazer/
]) compared to its estimated size during its red-giant phase in the future|alt=See caption]]
|title=SOHO Comets
The Sun does not have enough mass to explode as a ]. Instead, when it runs out of hydrogen in the core in approximately 5&nbsp;billion years, core hydrogen fusion will stop, and there will be nothing to prevent the core from contracting. The release of gravitational potential energy will cause the luminosity of the Sun to increase, ending the main sequence phase and leading the Sun to expand over the next billion years: first into a ], and then into a ].<ref name="carroll_ostlie" /><ref>{{cite web |first=Nola Taylor |last=Redd |title=Red Giant Stars: Facts, Definition & the Future of the Sun |url=http://www.space.com/22471-red-giant-stars.html |website=space.com |access-date=20 February 2016 |archive-date=9 February 2016 |archive-url=https://web.archive.org/web/20160209042249/http://www.space.com/22471-red-giant-stars.html |url-status=live }}</ref><ref name=schroder>{{Cite journal |last1=Schröder |first1=K.-P. |last2=Connon Smith |first2=R. |doi=10.1111/j.1365-2966.2008.13022.x |title=Distant future of the Sun and Earth revisited |journal=Monthly Notices of the Royal Astronomical Society |volume=386 |issue=1 |pages=155–163 |year=2008 |doi-access=free |arxiv=0801.4031 |bibcode=2008MNRAS.386..155S|s2cid=10073988 }}</ref> The heating due to gravitational contraction will also lead to expansion of the Sun and hydrogen fusion in a shell just outside the core, where unfused hydrogen remains, contributing to the increased luminosity, which will eventually reach more than 1,000 times its present luminosity.<ref name="carroll_ostlie" /> When the Sun enters its ] (RGB) phase, it will engulf (and very likely destroy) ] and ]. According to a 2008 paper, Earth's orbit will have initially expanded to at most {{Convert|1.5|AU|e6km e6mi|abbr=unit|sigfig=2}} due to the Sun's loss of mass. However, Earth's orbit will then start shrinking due to ] (and, eventually, drag from the lower chromosphere) so that it is engulfed by the Sun during the ] phase 7.59&nbsp;billion years from now, 3.8 and 1&nbsp;million years after Mercury and Venus have respectively suffered the same fate.<ref name="schroder" />
|accessdate=2006-03-22}}</ref>


By the time the Sun reaches the tip of the red-giant branch, it will be about 256 times larger than it is today, with a radius of {{Convert|1.19|AU|e6km e6mi|abbr=unit}}.<ref name="schroder" /><ref name="sackmann">{{Cite journal |last1=Boothroyd |first1=Arnold I. |last2=Sackmann |first2=I.-Juliana |date=January 1, 1999 |orig-date=19 December 1995 |title=The CNO Isotopes: Deep Circulation in Red Giants and First and Second Dredge-up |url=https://iopscience.iop.org/article/10.1086/306546 |journal=The Astrophysical Journal |publisher=The American Astronomical Society (AAS), The Institute of Physics (IOP) |volume=510 |issue=1 |pages=232–250 |arxiv=astro-ph/9512121 |bibcode=1999ApJ...510..232B |doi=10.1086/306546 |s2cid=561413}}</ref> The Sun will spend around a billion years in the RGB and lose around a third of its mass.<ref name="schroder" />
All these satellites have observed the Sun from the plane of the ecliptic, and so have only observed its equatorial regions in detail. The ] was launched in 1990 to study the Sun's polar regions. It first traveled to ], to 'slingshot' past the planet into an orbit which would take it far above the plane of the ecliptic. Serendipitously, it was well-placed to observe the collision of ] with Jupiter in 1994. Once Ulysses was in its scheduled orbit, it began observing the solar wind and magnetic field strength at high solar latitudes, finding that the solar wind from high latitudes was moving at about 750&nbsp;km/s (slower than expected), and that there were large magnetic waves emerging from high latitudes which scattered galactic ]s.<ref>{{cite web
|url=http://ulysses.jpl.nasa.gov/science/mission_primary.html
|title=Ulysses - Science - Primary Mission Results
|publisher=NASA
|accessdate=2006-03-22}}</ref>


After the red-giant branch, the Sun has approximately 120&nbsp;million years of active life left, but much happens. First, the core (full of ] helium) ignites violently in the ]; it is estimated that 6% of the core—itself 40% of the Sun's mass—will be converted into carbon within a matter of minutes through the ].<ref>{{Cite web | first=David | last=Taylor | publisher=Northwestern University | url=http://faculty.wcas.northwestern.edu/~infocom/The%20Website/end.html | title=The End Of The Sun | access-date=24 May 2015 | archive-date=22 May 2019 | archive-url=https://web.archive.org/web/20190522175414/http://faculty.wcas.northwestern.edu/~infocom/The%20Website/end.html | url-status=live}}</ref> The Sun then shrinks to around 10 times its current size and 50 times the luminosity, with a temperature a little lower than today. It will then have reached the ] or ], but a star of the Sun's metallicity does not evolve blueward along the horizontal branch. Instead, it just becomes moderately larger and more luminous over about 100&nbsp;million years as it continues to react helium in the core.<ref name=schroder />
Elemental abundances in the photosphere are well known from ] studies, but the composition of the interior of the Sun is more poorly understood. A ] sample return mission, ], was designed to allow astronomers to directly measure the composition of solar material. Genesis returned to ] in 2004 but was damaged by a crash landing after its ] failed to deploy on reentry into Earth's atmosphere. Despite severe damage, some usable samples have been recovered from the spacecraft's sample return module and are undergoing analysis.


When the helium is exhausted, the Sun will repeat the expansion it followed when the hydrogen in the core was exhausted. This time, however, it all happens faster, and the Sun becomes larger and more luminous. This is the ] phase, and the Sun is alternately reacting hydrogen in a shell or helium in a deeper shell. After about 20&nbsp;million years on the early asymptotic giant branch, the Sun becomes increasingly unstable, with rapid mass loss and ]s that increase the size and luminosity for a few hundred years every 100,000&nbsp;years or so. The thermal pulses become larger each time, with the later pulses pushing the luminosity to as much as 5,000 times the current level. Despite this, the Sun's maximum AGB radius will not be as large as its tip-RGB maximum: 179 {{Solar radius|link=yes}}, or about {{Convert|0.832|AU|e6km e6mi|abbr=unit}}.<ref name="schroder" /><ref name=agb>{{Cite journal |last1=Vassiliadis |first1=E. |last2=Wood |first2=P. R. |doi=10.1086/173033 |title=Evolution of low- and intermediate-mass stars to the end of the asymptotic giant branch with mass loss |journal=The Astrophysical Journal |volume=413 |page=641 |year=1993 |bibcode=1993ApJ...413..641V|doi-access=free }}</ref>
==Sun observation and eye damage==
]/EIT ] using ] light from the ] ] at ]&nbsp;].]]


Models vary depending on the rate and timing of mass loss. Models that have higher mass loss on the red-giant branch produce smaller, less luminous stars at the tip of the asymptotic giant branch, perhaps only 2,000 times the luminosity and less than 200 times the radius.<ref name="schroder" /> For the Sun, four thermal pulses are predicted before it completely loses its outer envelope and starts to make a ].<ref name=SunIII>{{cite journal |last1=Sackmann |first1=I.-J. |last2=Boothroyd |first2=A. I. |last3=Kraemer|first3=K. E. |date=1993 |title=Our Sun. III. Present and Future |journal=The Astrophysical Journal |volume=418 |pages=457–468 |doi=10.1086/173407 |bibcode=1993ApJ...418..457S}}</ref>
Sunlight is very bright, and looking directly at the Sun with the ] for brief periods can be painful, but is generally not hazardous. Looking directly at the Sun causes ] visual artifacts and temporary partial blindness. It also delivers about 4&nbsp;milliwatts of sunlight to the retina, slightly heating it and potentially (though not normally) damaging it. ] exposure gradually yellows the lens of the eye over a period of years and can cause ], but those depend on general exposure to solar UV, not on whether one looks directly at the Sun.


The post-asymptotic-giant-branch evolution is even faster. The luminosity stays approximately constant as the temperature increases, with the ejected half of the Sun's mass becoming ionized into a ] as the exposed core reaches {{Convert|30,000|K|F|sigfig=}}, as if it is in a sort of ]. The final naked core, a ], will have a temperature of over {{Convert|100,000|K|F|sigfig=}} and contain an estimated 54.05% of the Sun's present-day mass.<ref name=schroder /> (Simulations indicate that the Sun may be among the least massive stars capable of forming a planetary nebula.<ref>{{cite journal|last1=Gesicki |first1=K. |last2=Zijlstra |first2=A. A. |last3=Miller Bertolami |first3=M. M. |year=2018 |title=The mysterious age invariance of the planetary nebula luminosity function bright cut-off |journal=Nature Astronomy |volume=2 |number=7 |pages=580–584 |doi=10.1038/s41550-018-0453-9|arxiv=1805.02643 |bibcode=2018NatAs...2..580G }}</ref>) The planetary nebula will disperse in about 10,000&nbsp;years, but the white dwarf will survive for trillions of years before fading to a hypothetical super-dense ].<ref name=bloecker1>{{Cite journal |bibcode=1995A&A...297..727B |title=Stellar evolution of low and intermediate-mass stars. I. Mass loss on the AGB and its consequences for stellar evolution |last=Bloecker |first=T. |journal=Astronomy and Astrophysics |year=1995 |volume=297 |page=727}}</ref><ref name=bloecker2>{{Cite journal |bibcode = 1995A&A...299..755B |title=Stellar evolution of low- and intermediate-mass stars. II. Post-AGB evolution |last=Bloecker |first=T.|journal=Astronomy and Astrophysics |year=1995 |volume=299 |page=755}}</ref><ref>{{cite journal|first=Jørgen |last=Christensen-Dalsgaard |title=Solar structure and evolution |journal=Living Reviews in Solar Physics |year=2021 |volume=18 |number=2 |page=2 |doi=10.1007/s41116-020-00028-3|arxiv=2007.06488 |bibcode=2021LRSP...18....2C }}</ref> As such, it would give off no more energy.<ref name="Johnson-Groh 2020 j255">{{cite web | last=Johnson-Groh | first=Mara | title=The end of the universe may be marked by 'black dwarf supernova' explosions | website=Live Science | date=August 25, 2020 | url=https://www.livescience.com/black-dwarf-supernovae-end-universe.html | access-date=November 24, 2023 | archive-date=2 June 2023 | archive-url=https://web.archive.org/web/20230602022731/https://www.livescience.com/black-dwarf-supernovae-end-universe.html | url-status=live }}</ref>
Viewing the Sun through light-concentrating ] such as ] is very hazardous without an ] to dim the sunlight. Unfiltered binoculars can deliver over 500 times more sunlight to the retina than does the naked eye, killing retinal cells almost instantly. Even brief glances at the midday Sun through unfiltered binoculars can cause permanent blindness.<ref name="Marsh">{{cite journal
|last=Marsh
|first=J. C. D.
|url=http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1982JBAA...92..257M&amp;data_type=PDF_HIGH&amp;type=PRINTER&amp;filetype=.pdf
|title=Observing the Sun in Safety
|journal=J. Brit. Ast. Assoc.
|year=1982
|volume=92
|pages=6}}</ref> One way to view the Sun safely is by projecting an image onto a screen using binoculars. This should only be done with a small refracting telescope (or binoculars) with a clean eyepiece. Other kinds of telescope can be damaged by this procedure.


== Location ==
Partial ]s are hazardous to view because the eye's ] is not adapted to the unusually high visual contrast: the pupil dilates according to the total amount of light in the field of view, ''not'' by the brightest object in the field. During partial eclipses most sunlight is blocked by the Moon passing in front of the Sun, but the uncovered parts of the photosphere have the same ] as during a normal day. In the overall gloom, the pupil expands from ~2&nbsp;mm to ~6&nbsp;mm, and each retinal cell exposed to the solar image receives about ten times more light than it would looking at the non-eclipsed Sun. This can damage or kill those cells, resulting in small permanent blind spots for the viewer.<ref name="Espenak">{{cite web
=== Solar System ===
|last=Espenak
{{Main|Solar System}}
|first=F.
], which extends to the edge of the ], where at {{val|125,000|fmt=commas|u=AU}} to {{val|230,000|fmt=commas|u=AU}}, equal to several light-years, the Sun's ] ends.]]
|title=Eye Safety During Solar Eclipses - adapted from NASA RP 1383 Total Solar Eclipse of 1998 February 26, April 1996, p. 17
The Sun has eight known planets orbiting it. This includes four ] (], ], ], and ]), two ] (] and ]), and two ] (] and ]). The Solar System also has nine bodies generally considered as ]s and some more ], an ], numerous ], and a large number of icy bodies which lie beyond the orbit of Neptune. Six of the planets and many smaller bodies also have their own ]s: in particular, the satellite systems of Jupiter, Saturn, and Uranus are in some ways like miniature versions of the Sun's system.<ref>{{cite book |title=Physics and Chemistry of the Solar System |date=2004 |publisher=Elsevier |editor-first=John |editor-last=Lewis |edition=2 |page=265 | isbn=9780080470122 | url=https://books.google.com/books?id=xl50rOf5V08C&pg=PA265 }}</ref>
|url=http://sunearth.gsfc.nasa.gov/eclipse/SEhelp/safety.html
|accessdate=2006-03-22
|publisher=NASA}}</ref> The hazard is insidious for inexperienced observers and for children, because there is no perception of pain: it is not immediately obvious that one's vision is being destroyed.


The Sun is moved by the gravitational pull of the planets. The center of the Sun moves around the Solar System ], within a range from 0.1 to 2.2 solar radii. The Sun's motion around the barycenter approximately repeats every 179&nbsp;years, rotated by about 30° due primarily to the ] of Jupiter and Saturn.<ref>{{cite journal |first=Paul D. | last=Jose |title=Sun's Motion and Sunspots |journal=] |date=Apr 1965 |volume=70 | issue=3 |pages=193–200 |doi=10.1086/109714 |bibcode=1965AJ.....70..193J |url=http://www.landscheidt.info/pdf/jose1965.pdf |access-date=22 March 2020 |archive-date=22 March 2020 |archive-url=https://web.archive.org/web/20200322184010/http://www.landscheidt.info/pdf/jose1965.pdf |url-status=live }}</ref>
During ] and ], sunlight is attenuated through ] and ] of light by a particularly long passage through Earth's atmosphere, and the direct Sun is sometimes faint enough to be viewed directly without discomfort or safely with binoculars (provided there is no risk of bright sunlight suddenly appearing in a break between clouds). Hazy conditions, atmospheric dust, and high humidity contribute to this atmospheric attenuation.


The Sun's gravitational field is estimated to ] out to about two light-years ({{val|125,000|fmt=commas|u=AU}}). Lower estimates for the radius of the ], by contrast, do not place it farther than {{val|50,000|fmt=commas|u=AU}}.<ref name="Encrenaz_et_al_2004">{{Cite book |last1=Encrenaz |first1=T. |author-link=Thérèse Encrenaz |title=The Solar System |last2=Bibring |first2=J. P. |last3=Blanc |first3=M. |last4=Barucci |first4=M. A. |last5=Roques |first5=F. |last6=Zarka |first6=P. H. |date=2004 |publisher=Springer |edition=3rd |page=1}}</ref> Most of the mass is orbiting in the region between 3,000 and {{val|100,000|fmt=commas|u=AU}}.<ref>{{Cite journal |last1=Torres |first1=S. |last2=Cai |first2=M. X. |last3=Brown |first3=A. G. A. |last4=Portegies Zwart |first4=S. |date=September 2019 |title=Galactic tide and local stellar perturbations on the Oort cloud: creation of interstellar comets |journal=Astronomy & Astrophysics |volume=629 |page=13 |arxiv=1906.10617 |bibcode=2019A&A...629A.139T |doi=10.1051/0004-6361/201935330 |s2cid=195584070 |id=A139}}</ref> The furthest known objects, such as ], have aphelia around {{val|70,000|fmt=commas|u=AU}} from the Sun.<ref>{{Cite web |last=Norman |first=Neil |date=May 2020 |title=10 great comets of recent times |url=https://www.skyatnightmagazine.com/space-science/greatest-comets-of-recent-times |url-status=live |archive-url=https://web.archive.org/web/20220125042109/https://www.skyatnightmagazine.com/space-science/greatest-comets-of-recent-times |archive-date=25 January 2022 |access-date=10 April 2022 |website=]}}</ref> The Sun's ] with respect to the galactic nucleus, the effective range of its gravitational influence, is thought to extend up to a thousand times farther and encompasses the hypothetical Oort cloud.<ref name="Littmann">{{Cite book |last=Littmann |first=Mark |url=https://archive.org/details/planetsbeyonddis00mlit |title=Planets Beyond: Discovering the Outer Solar System |date=2004 |publisher=Courier Dover Publications |isbn=978-0-486-43602-9 |pages=–163 |url-access=limited}}</ref> It was calculated by ] to be 230,000&nbsp;AU.<ref name="Chebotarev">{{cite journal |last1=Chebotarev |first1=G. A. |title=Gravitational Spheres of the Major Planets, Moon and Sun |journal=Astronomicheskii Zhurnal |date=1 January 1963 |volume=40 |pages=812 |bibcode=1964SvA.....7..618C |url=https://adsabs.harvard.edu/full/1964SvA.....7..618C |issn=0004-6299 |access-date=6 May 2024 |archive-date=7 May 2024 |archive-url=https://web.archive.org/web/20240507030847/https://adsabs.harvard.edu/full/1964SvA.....7..618C |url-status=live }}</ref>
Attenuating filters to view the Sun should be specifically designed for that use: some improvised filters pass UV or IR rays that can harm the eye at high brightness levels. In general, filters on telescopes or binoculars should be on the ] or ] rather than on the ], because eyepiece filters can suddenly shatter due to high heat loads from the absorbed sunlight. Welding glass is an acceptable solar filter, but "black" exposed photographic film is not (it passes too much infrared).


=== Celestial neighborhood ===
==Sun in human culture==
{{Excerpt|Solar System|Celestial neighborhood}}
Many civilizations have viewed the Sun as a sacred body. In ] religious literature, the Sun is notably mentioned as the visible form of ] that one can see every day. In ], ] (Devanagari: सूर्य, sūrya) is the chief solar deity, son of Dyaus Pitar. The ritual of ], performed by some ]s, is meant to worship the sun. The Sun was also worshiped in ], ] and ] culture.<ref></ref>


== Motion ==
Many Greek ] personify the Sun as a ] named ], who wore a shining crown and rode a ] across the sky, causing day. Over time, the sun became increasingly associated with ].
{{main|Galactic year}}
{{Further|Stellar kinematics}}
]


The Sun, taking along the whole Solar System, orbits ] at an average speed of 230&nbsp;km/s (828,000&nbsp;km/h) or 143&nbsp;mi/s (514,000&nbsp;mph),<ref name="StarChild">{{cite web |url=http://starchild.gsfc.nasa.gov/docs/StarChild/questions/question18.html |website=NASA |title=StarChild Question of the Month – Does the Sun move around the Milky Way? |date=February 2000 |url-status=live |archive-url=https://web.archive.org/web/20231030090914/https://starchild.gsfc.nasa.gov/docs/StarChild/questions/question18.html |archive-date= Oct 30, 2023 }}</ref> taking about 220–250&nbsp;million ]s to complete a revolution (a ]),<ref name="Siegel 2018 n418">{{cite web | last=Siegel | first=Ethan | title=Our Motion Through Space Isn't A Vortex, But Something Far More Interesting | website=Forbes | date=August 30, 2018 | url=https://www.forbes.com/sites/startswithabang/2018/08/30/our-motion-through-space-isnt-a-vortex-but-something-far-more-interesting/ | access-date=November 25, 2023 |url-status=live |archive-url=https://web.archive.org/web/20231125013457/https://www.forbes.com/sites/startswithabang/2018/08/30/our-motion-through-space-isnt-a-vortex-but-something-far-more-interesting/?sh=1cfdeca37ec2 |archive-date=November 25, 2023 }}</ref> having done so about 20 times since the Sun's formation.<ref name="Currin 2020 t043">{{cite web | last=Currin | first=Grant | title=How long is a galactic year? | website=Live Science | date=August 30, 2020 | url=https://www.livescience.com/how-long-galactic-year.html | access-date=November 25, 2023 | archive-date=25 November 2023 | archive-url=https://web.archive.org/web/20231125013457/https://www.livescience.com/how-long-galactic-year.html | url-status=live }}</ref><ref name="fn10">{{cite web |last=Leong |first=S. |title=Period of the Sun's Orbit around the Galaxy (Cosmic Year) |url=http://hypertextbook.com/facts/2002/StacyLeong.shtml |website=The Physics Factbook |date=2002 |access-date=10 May 2007 |archive-date=22 August 2011 |archive-url=https://www.webcitation.org/617GgQWCh?url=http://hypertextbook.com/facts/2002/StacyLeong.shtml |url-status=live }}</ref> The direction of the Sun's motion, the ], is roughly in the direction of the star ].<ref>{{cite book | title=Three Hundred and Sixty Five Starry Nights: An Introduction to Astronomy for Every Night of the Year | first=Chet | last=Raymo | year=1990 | publisher=Touchstone | isbn=9780671766061 | url=https://books.google.com/books?id=rTe5HaRsAS4C&pg=PA114 }}</ref>
The ] adopted Helios into their own mythology as ]. The title ] ("the undefeated Sun") was applied to several solar deities, and depicted on several types of Roman ] during the ] and ].


]
Early Christian ] reveals ] as reflecting several attributes of Sol Invictus, such as a radiated ] or, occasionally, a solar chariot. ] that the observation of ] on ] is derived from a ] Sun holiday which occurred on the same date.


The Milky Way is moving with respect to the ] (CMB) in the direction of the constellation ] with a speed of 550&nbsp;km/s. Since the sun is moving with respect to the galactic center in the direction of Cygnus (galactic longitude 90°; latitude 0°) at more than 200{{nbsp}}km/sec, the resultant velocity with respect to the CMB is about 370&nbsp;km/s in the direction of ] or ] (galactic latitude 264°, latitude 48°).<ref>Table 3 of {{Cite journal |last=Kogut |first=A. |date=1993 |title=Dipole Anisotropy in the COBE Differential Microwave Radiometers First-Year Sky Maps |journal=] |volume=419 |issue=1993 |page=1 |arxiv=astro-ph/9312056 |doi=10.1086/173453 |bibcode=1993ApJ...419....1K |display-authors=etal}}</ref>
: ''See also: ]''


== Observational history ==
==See also==
* ]
* ]


=== Early understanding ===
==References==
{{See also|The Sun in culture}}
<div class="references-small">
] pulled by a horse is a sculpture believed to be illustrating an important part of ] mythology.|alt=A sculpture of the sun in a chariot being pulled by a horse that has wheels instead of hoofs.]]
<references/>
In many prehistoric and ancient cultures, the Sun was thought to be a solar deity or other ] entity.<ref name="e488">{{cite book | last=Hawthorn | first=Hannah | title=The Magick of Birthdays | publisher=Penguin | publication-place=New York | date=2022 | isbn=978-0-593-53854-8 | page=103}}</ref><ref name="t793">{{cite book | last=Singh | first=Madanjeet | title=The Sun | publisher=ABRAMS | publication-place=New York | date=1993 | isbn=978-0-8109-3838-0 | page=305}}</ref> In the early first millennium BC, ] observed that the Sun's motion along the ] is not uniform, though they did not know why; it is today known that this is due to the movement of Earth in an ], moving faster when it is nearer to the Sun at perihelion and moving slower when it is farther away at aphelion.<ref>{{Cite book |title=Babylon to Voyager and beyond: a history of planetary astronomy |first=David |last=Leverington |publisher=] |date=2003 |isbn=978-0-521-80840-8 |pages=6–7}}</ref>
* Thompson, M. J. (2004), ''Solar interior: Helioseismology and the Sun's interior'', Astronomy & Geophysics, v. 45, p. 4.21-4.25
* T. J. White; M. A. Mainster; P. W. Wilson; and J. H. Tips, ''Chorioretinal temperature increases from solar observation'', Bulletin of Mathematical Biophysics 33, 1-17 (1971)
</div>
*^biman basu- space quiz. published by scholastic india pvt. ltd.


One of the first people to offer a scientific or philosophical explanation for the Sun was the ] philosopher ]. He reasoned that it was a giant flaming ball of metal even larger than the land of the ] and that the Moon reflected the light of the Sun.<ref>{{Cite journal |last=Sider |first=D. |title=Anaxagoras on the Size of the Sun |jstor=269068 |journal=] |volume=68 |issue=2 |pages=128–129 |date=1973 |doi=10.1086/365951|s2cid=161940013 }}</ref> ] estimated the distance between Earth and the Sun in the third century BC as "of stadia ]s 400 and 80000", the translation of which is ambiguous, implying either 4,080,000 ] (755,000&nbsp;km) or 804,000,000 stadia (148 to 153&nbsp;million kilometers or 0.99 to 1.02 AU); the latter value is correct to within a few percent. In the first century AD, ] estimated the distance as 1,210 times ], approximately {{convert|{{#expr:1.210*6.371round2}}|e6km|AU|sp=us}}.<ref>{{Cite journal |last=Goldstein |first=B. R. |title=The Arabic Version of Ptolemy's Planetary Hypotheses |journal=Transactions of the American Philosophical Society |volume=57 |issue=4 |pages=9–12 |date=1967 |doi=10.2307/1006040|jstor=1006040}}</ref>
==External links==
{{sisterlinks|Sun}}
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* from
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* from
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* and from the
* - a celestial mechanics and astronomical calculation library
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The theory that the Sun is the center around which the planets orbit was first proposed by the ancient Greek ] in the third century BC,<ref>{{Cite journal |last=Stahl |first=William Harris |date=1945 |title=The Greek Heliocentric Theory and Its Abandonment |jstor=283344 |journal=Transactions and Proceedings of the American Philological Association |volume=76 |pages=321–332 |doi=10.2307/283344 |issn=0065-9711}}</ref> and later adopted by ] (see ]).<ref>{{cite book |last=Toomer |first=G. J. |chapter=Seleucus (5), of Seleuceia, astronomer |date=2016-03-07 |title=Oxford Research Encyclopedia of Classics |url=https://oxfordre.com/classics/view/10.1093/acrefore/9780199381135.001.0001/acrefore-9780199381135-e-5799 |access-date=2024-05-27 |publisher=Oxford University Press |doi=10.1093/acrefore/9780199381135.013.5799 |isbn=978-0-19-938113-5}}</ref> This view was developed in a more detailed mathematical model of a heliocentric system in the 16th century by ].<ref>{{Cite book |last1=Fraknoi |first1=Andrew |last2=Morrison |first2=David |last3=Wolff |first3=Sidney |date=2022-03-09 |chapter=2.4 The Birth of Modern Astronomy |title=Astronomy 2e |publisher=OpenStax |chapter-url=https://openstax.org/books/astronomy-2e/pages/2-4-the-birth-of-modern-astronomy |access-date=2024-05-27}}</ref>
{{Footer Sun}}
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=== Development of scientific understanding ===
]
]'s ''Liber astronomiae''|alt=A drawing of a man wearing a crown in a chariot, being pulled by horses.]]
]
Observations of sunspots were recorded during the ] (206 BC–AD 220) by ], who maintained records of these observations for centuries. ] also provided a description of sunspots in the 12th century.<ref>{{cite book |last=Ead |first=Hamed A. |title=Averroes As A Physician |publisher=] | url=https://www.alchemywebsite.com/islam21.html | year=1998 | access-date=2024-05-27 }}</ref> The invention of the telescope in the early 17th century permitted detailed observations of sunspots by ], ] and other astronomers. Galileo posited that sunspots were on the surface of the Sun rather than small objects passing between Earth and the Sun.<ref>{{cite web |title=Galileo Galilei (1564–1642) |url=https://www.bbc.co.uk/history/historic_figures/galilei_galileo.shtml |publisher=BBC |access-date=22 March 2006 |archive-date=29 September 2018 |archive-url=https://web.archive.org/web/20180929134432/http://www.bbc.co.uk/history/historic_figures/galilei_galileo.shtml |url-status=live }}</ref>
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] include ]'s discovery that the direction of the Sun's ] (the place in the Sun's orbit against the fixed stars where it seems to be moving slowest) is changing.<ref>{{cite book|title=A short History of scientific ideas to 1900 |first=C. |last=Singer |publisher=Oxford University Press |year=1959 |page=151}}</ref> (In modern heliocentric terms, this is caused by a gradual motion of the aphelion of the ''Earth's'' orbit). ] observed more than 10,000 entries for the Sun's position for many years using a large ].<ref>{{cite book | chapter=The Arabian Science | first=C. | last=Ronan | pages=201–244 | title=The Cambridge Illustrated History of the World's Science | publisher=Cambridge University Press | year=1983 }} at pp. 213–214.</ref>
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From an observation of a ] in 1032, the Persian astronomer and polymath ] concluded that Venus was closer to Earth than the Sun.<ref name=Goldstein>{{Cite journal |title=Theory and Observation in Medieval Astronomy |first=Bernard R. |last=Goldstein |journal=] |volume=63 |issue=1 |date=March 1972 |pages=39–47 |doi=10.1086/350839|bibcode=1972Isis...63...39G |s2cid=120700705 }}</ref> In 1677, ] observed a transit of Mercury across the Sun, leading him to realize that observations of the ] of a planet (more ideally using the transit of Venus) could be used to ] determine the distances between Earth, ], and the Sun.<ref>{{Cite conference |last=Chapman |first=Allan |date=April 2005 |editor-last=Kurtz |editor-first=D. W. |title=Jeremiah Horrocks, William Crabtree, and the Lancashire observations of the transit of Venus of 1639 |conference=Transits of Venus: New Views of the Solar System and Galaxy, Proceedings of IAU Colloquium #196, held 7–11 June 2004 in Preston, U.K. |publisher=Cambridge University Press |publication-place=Cambridge |volume=2004 |pages=3–26 |bibcode=2005tvnv.conf....3C |doi=10.1017/S1743921305001225 |doi-access=free |journal=Proceedings of the International Astronomical Union}}</ref> Careful observations of the ] allowed astronomers to calculate the average Earth–Sun distance as {{Convert|93726900|mi|km}}, only 0.8% greater than the modern value.<ref>{{Cite journal |last=Teets |first=Donald |date=December 2003 |title=Transits of Venus and the Astronomical Unit |url=http://www.maa.org/sites/default/files/pdf/pubs/mm_dec03-Venus.pdf |url-status=live |journal=Mathematics Magazine |volume=76 |pages=335–348 |doi=10.1080/0025570X.2003.11953207 |jstor=3654879 |s2cid=54867823 |archive-url=https://web.archive.org/web/20220203080207/https://www.maa.org/sites/default/files/pdf/pubs/mm_dec03-Venus.pdf |archive-date=3 February 2022 |access-date=3 April 2022 |number=5}}</ref>
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In 1666, ] observed the Sun's light using a ], and showed that it is made up of light of many colors.<ref>{{cite news |title=Sir Isaac Newton (1643–1727) |newspaper=BBC Teach |url=https://www.bbc.co.uk/history/historic_figures/newton_isaac.shtml |publisher=BBC |access-date=22 March 2006 |archive-date=10 March 2015 |archive-url=https://web.archive.org/web/20150310093436/http://www.bbc.co.uk/history/historic_figures/newton_isaac.shtml |url-status=live }}</ref> In 1800, ] discovered ] radiation beyond the red part of the solar spectrum.<ref>{{cite web |title=Herschel Discovers Infrared Light |url=http://coolcosmos.ipac.caltech.edu/cosmic_classroom/classroom_activities/herschel_bio.html |publisher=Cool Cosmos |access-date=22 March 2006 |url-status=dead |archive-url=https://web.archive.org/web/20120225094516/http://coolcosmos.ipac.caltech.edu/cosmic_classroom/classroom_activities/herschel_bio.html |archive-date=25 February 2012 }}</ref> The 19th century saw advancement in spectroscopic studies of the Sun; ] recorded more than 600 ] in the spectrum, the strongest of which are still often referred to as ]. The 20th century brought about several specialized systems for observing the Sun, especially at different narrowband wavelengths, such as those using Calcium H (396.9&nbsp;nm), K (393.37&nbsp;nm) and ] (656.46&nbsp;nm) ].<ref>{{cite book
]
| chapter=Instruments for observing the Corona
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| first=Gudrun | last=Wolfschmidt
]
| title=Instruments of Science, An Historical Encyclopedia
]
| year=1998 | pages=147–148 | isbn=9780815315612
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| publisher=Science Museum, London, and National Museum of American History, Smithsonian Institution
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| editor1-first=Deborah Jean | editor1-last=Warner
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| editor2-first=Robert | editor2-last=Bud
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| chapter-url=https://books.google.com/books?id=1AsFdUxOwu8C&pg=PA148 }}</ref>
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During early studies of the ] of the photosphere, some absorption lines were found that did not correspond to any ]s then known on Earth. In 1868, ] hypothesized that these absorption lines were caused by a new element that he dubbed ''helium'', after the Greek Sun god ]. Twenty-five years later, helium was isolated on Earth.<ref name="Lockyer">{{Cite web |last=Parnel |first=C. |title=Discovery of Helium |url=http://www-solar.mcs.st-andrews.ac.uk/~clare/Lockyer/helium.html |url-status=live |archive-url=https://web.archive.org/web/20151107043457/http://www-solar.mcs.st-andrews.ac.uk/~clare/Lockyer/helium.html |archive-date=7 November 2015 |access-date=22 March 2006 |publisher=University of St Andrews}}</ref>
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In the early years of the modern scientific era, the source of the Sun's energy was a significant puzzle. ] suggested that the Sun is a gradually cooling liquid body that is radiating an internal store of heat.<ref name=kelvin>{{Cite journal |last=Thomson |first=W. |title=On the Age of the Sun's Heat |url=http://zapatopi.net/kelvin/papers/on_the_age_of_the_suns_heat.html |journal=] |date=1862 |volume=5 |pages=388–393 |access-date=25 August 2006 |archive-date=25 September 2006 |archive-url=https://web.archive.org/web/20060925190954/http://zapatopi.net/kelvin/papers/on_the_age_of_the_suns_heat.html |url-status=live }}</ref> Kelvin and ] then proposed a ] mechanism to explain the energy output, but the resulting age estimate was only 20&nbsp;million years, well short of the time span of at least 300&nbsp;million years suggested by some geological discoveries of that time.<ref name=kelvin /><ref>{{cite journal |year=2000 |title=Kelvin's age of the Earth paradox revisited |journal=] |volume=105 |issue=B6 |pages=13155–13158 |bibcode=2000JGR...10513155S |doi=10.1029/2000JB900028 |last1=Stacey |first1=Frank D.|doi-access=free }}</ref><!-- In XIX century, before discovery of radionuclear dating, there was no reason to suggest that Earth exists for as long as 4 billion years. --> In 1890, Lockyer proposed a meteoritic hypothesis for the formation and evolution of the Sun.<ref>{{Cite journal |last=Lockyer |first=J. N. |title=The meteoritic hypothesis; a statement of the results of a spectroscopic inquiry into the origin of cosmical systems |journal=London and New York |year=1890 |bibcode=1890mhsr.book.....L}}</ref>
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Not until 1904 was a documented solution offered. ] suggested that the Sun's output could be maintained by an internal source of heat, and suggested ] as the source.<ref>{{cite web |last=Darden |first=L. |title=The Nature of Scientific Inquiry |url=http://www.philosophy.umd.edu/Faculty/LDarden/sciinq/ |year=1998 |access-date=25 August 2006 |archive-date=17 August 2012 |archive-url=https://web.archive.org/web/20120817040843/http://www.philosophy.umd.edu/Faculty/LDarden/sciinq/ |url-status=live }}</ref> However, it would be ] who would provide the essential clue to the source of the Sun's energy output with his ] relation {{nowrap|''E'' {{=}} ''mc''<sup>2</sup>}}.<ref>{{Cite book |last=Hawking |first=S. W. |author-link = Stephen Hawking |date=2001 |title=The Universe in a Nutshell |publisher=Bantam |isbn=978-0-553-80202-3 | page=12 | url=https://books.google.com/books?id=0CO2iwfzRJkC&pg=PA12 }}</ref> In 1920, Sir ] proposed that the pressures and temperatures at the core of the Sun could produce a nuclear fusion reaction that merged hydrogen (protons) into helium nuclei, resulting in a production of energy from the net change in mass.<ref>{{cite web |title=Studying the stars, testing relativity: Sir Arthur Eddington |url=http://www.esa.int/esaSC/SEMDYPXO4HD_index_0.html |website=Space Science |publisher=] |date=2005 |access-date=1 August 2007 |archive-date=20 October 2012 |archive-url=https://web.archive.org/web/20121020174459/http://www.esa.int/esaSC/SEMDYPXO4HD_index_0.html |url-status=live }}</ref> The preponderance of hydrogen in the Sun was confirmed in 1925 by ] using the ionization theory developed by ]. The theoretical concept of fusion was developed in the 1930s by the astrophysicists ] and ]. Hans Bethe calculated the details of the two main energy-producing nuclear reactions that power the Sun.<ref name="Bethe">{{Cite journal |last1=Bethe |first1=H. |title=On the Formation of Deuterons by Proton Combination |journal=] |volume=54 |issue=10 |page=862 |date=1938 |doi=10.1103/PhysRev.54.862.2 |last2=Critchfield |first2=C.|bibcode=1938PhRv...54Q.862B}}</ref><ref name="Bethe2">{{Cite journal |last=Bethe |first=H. |title=Energy Production in Stars |journal=] |volume=55 |issue=1 |pages=434–456 |date=1939 |doi=10.1103/PhysRev.55.434 |pmid=17835673|bibcode=1939PhRv...55..434B|s2cid=36146598 |doi-access=free }}</ref> In 1957, ], ], ] and ] showed that most of the elements in the universe have been ] by nuclear reactions inside stars, some like the Sun.<ref>{{Cite journal |first1=E. M. |last1=Burbidge |first2=G. R. |last2=Burbidge |first3=W. A. |last3=Fowler |first4=F. |last4=Hoyle |title=Synthesis of the Elements in Stars |journal=] |volume=29 |issue=4 |pages=547–650 | year=1957 |doi=10.1103/RevModPhys.29.547 |bibcode=1957RvMP...29..547B |url=https://authors.library.caltech.edu/45747/1/BURrmp57.pdf |doi-access=free |access-date=12 April 2020 |archive-date=23 July 2018 |archive-url=https://web.archive.org/web/20180723054833/https://authors.library.caltech.edu/45747/1/BURrmp57.pdf |url-status=live }}</ref>
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=== Solar space missions ===
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{{See also|Solar observatory|List of heliophysics missions}}
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]|alt=See caption]]
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The first satellites designed for long term observation of the Sun from interplanetary space were NASA's ] 6, 7, 8 and 9, which were launched between 1959 and 1968. These probes orbited the Sun at a distance similar to that of Earth, and made the first detailed measurements of the solar wind and the solar magnetic field. ] operated for a particularly long time, transmitting data until May 1983.<ref>{{cite web |last=Wade |first=M. |title=Pioneer 6-7-8-9-E |url=http://www.astronautix.com/craft/pio6789e.htm |date=2008 |publisher=] |access-date=22 March 2006 |url-status=dead |archive-url=https://web.archive.org/web/20060422075141/http://www.astronautix.com/craft/pio6789e.htm |archive-date=22 April 2006 |df=dmy-all}}</ref><ref>{{cite web |title=Solar System Exploration: Missions: By Target: Our Solar System: Past: Pioneer 9 |url=http://solarsystem.nasa.gov/missions/profile.cfm?MCode=Pioneer_09 |publisher=] |access-date=30 October 2010 |quote=NASA maintained contact with Pioneer 9 until May 1983 |url-status=dead |archive-url=https://web.archive.org/web/20120402205810/http://solarsystem.nasa.gov/missions/profile.cfm?MCode=Pioneer_09 |archive-date=2 April 2012 |df=dmy-all}}</ref>
]

]
In the 1970s, two ] and the Skylab ] provided scientists with significant new data on solar wind and the solar corona. The Helios 1 and 2 probes were U.S.–German collaborations that studied the solar wind from an orbit carrying the spacecraft inside Mercury's orbit at perihelion.<ref name=Burlaga2001 /> The Skylab space station, launched by NASA in 1973, included a solar observatory module called the Apollo Telescope Mount that was operated by astronauts resident on the station.<ref name=Dwivedi2006 /> Skylab made the first time-resolved observations of the solar transition region and of ultraviolet emissions from the solar corona.<ref name=Dwivedi2006 /> Discoveries included the first observations of coronal mass ejections, then called "coronal transients", and of ]s, now known to be intimately associated with the solar wind.<ref name=Burlaga2001>{{Cite journal |last=Burlaga |first=L. F. |title=Magnetic Fields and plasmas in the inner heliosphere: Helios results | year=2001 |journal=Planetary and Space Science |volume=49 |issue=14–15 |pages=1619–1627 |doi=10.1016/S0032-0633(01)00098-8 |bibcode=2001P&SS...49.1619B |url=https://zenodo.org/record/1259695 |access-date=25 August 2019 |archive-date=13 July 2020 |archive-url=https://web.archive.org/web/20200713051926/https://zenodo.org/record/1259695 |url-status=live }}</ref>
]
] probe|alt=See caption]]
]
In 1980, the ] probes were launched by NASA. This spacecraft was designed to observe gamma rays, ]s and ] radiation from solar flares during a time of high solar activity and solar luminosity. Just a few months after launch, however, an electronics failure caused the probe to go into standby mode, and it spent the next three years in this inactive state. In 1984, ] mission ] retrieved the satellite and repaired its electronics before re-releasing it into orbit. The Solar Maximum Mission subsequently acquired thousands of images of the solar corona before ] Earth's atmosphere in June 1989.<ref>{{cite web |last=Burkepile |first=C. J. |title=Solar Maximum Mission Overview |url=http://web.hao.ucar.edu/public/research/svosa/smm/smm_mission.html |date=1998 |access-date=22 March 2006 |archive-url=https://web.archive.org/web/20060405183758/http://web.hao.ucar.edu/public/research/svosa/smm/smm_mission.html |archive-date=5 April 2006}}</ref>
]

]
Launched in 1991, Japan's ] (''Sunbeam'') satellite observed solar flares at X-ray wavelengths. Mission data allowed scientists to identify several different types of flares and demonstrated that the corona away from regions of peak activity was much more dynamic and active than had previously been supposed. Yohkoh observed an entire solar cycle but went into standby mode when an annular eclipse in 2001 caused it to lose its lock on the Sun. It was destroyed by atmospheric re-entry in 2005.<ref>{{cite press release |title=Result of Re-entry of the Solar X-ray Observatory "Yohkoh" (SOLAR-A) to the Earth's Atmosphere |url=http://www.jaxa.jp/press/2005/09/20050913_yohkoh_e.html |publisher=] | date=13 September 2005 |access-date=22 March 2006 |archive-date=10 August 2013 |archive-url=https://web.archive.org/web/20130810150641/http://www.jaxa.jp/press/2005/09/20050913_yohkoh_e.html |url-status=dead }}</ref>
]

]
The ], jointly built by the ] and NASA, was launched on 2 December 1995.<ref name=Dwivedi2006 /> Originally intended to serve a two-year mission,<ref>{{cite web|url=https://www.universetoday.com/138664/22-years-of-the-sun-from-soho/ |title=22 Years of the Sun from SOHO |website=Universe Today |access-date=31 May 2024 |date=26 February 2018 |first=Evan |last=Gough}}</ref> SOHO remains in operation as of 2024.<ref>{{cite web|url=https://www.universetoday.com/166353/someone-just-found-sohos-5000th-comet/ |title=Someone Just Found SOHO's 5,000th Comet |first=Nancy |last=Atkinson |date=28 March 2024 |access-date=31 May 2024 |website=Universe Today}}</ref> Situated at the ] between Earth and the Sun (at which the gravitational pull from both is equal), SOHO has provided a constant view of the Sun at many wavelengths since its launch.<ref name=Dwivedi2006 /> Besides its direct solar observation, SOHO has enabled the discovery of a large number of ]s, mostly tiny ]s that incinerate as they pass the Sun.<ref>{{cite web |title=Sungrazing Comets |url=http://sungrazer.nrl.navy.mil/ |publisher=] (]) | date=13 March 2015 |access-date=19 March 2009 |archive-date=25 May 2015 |archive-url=https://web.archive.org/web/20150525060147/http://sungrazer.nrl.navy.mil/ |url-status=live }}</ref>
]
] testing at the vacuum spin-balancing facility|alt=A photograph of Ulysses spacecraft]]
]
]|alt=See caption]]
]
All these satellites have observed the Sun from the plane of the ecliptic, and so have only observed its equatorial regions in detail. The ] was launched in 1990 to study the Sun's polar regions. It first traveled to Jupiter, to "slingshot" into an orbit that would take it far above the plane of the ecliptic. Once ''Ulysses'' was in its scheduled orbit, it began observing the solar wind and magnetic field strength at high solar latitudes, finding that the solar wind from high latitudes was moving at about 750&nbsp;km/s, which was slower than expected, and that there were large magnetic waves emerging from high latitudes that scattered galactic cosmic rays.<ref>{{cite web |author=]/] |title=Ulysses: Primary Mission Results |url=http://ulysses.jpl.nasa.gov/science/mission_primary.html |publisher=NASA | year=2005 |access-date=22 March 2006 |url-status=dead |archive-url=https://web.archive.org/web/20060106150819/http://ulysses.jpl.nasa.gov/science/mission_primary.html |archive-date=6 January 2006 }}</ref>
]

]
Elemental abundances in the photosphere are well known from ] studies, but the composition of the interior of the Sun is more poorly understood. A solar wind sample return mission, '']'', was designed to allow astronomers to directly measure the composition of solar material.<ref>{{Cite journal |last1=Calaway |first1=M. J. |title=Genesis capturing the Sun: Solar wind irradiation at Lagrange 1 |journal=] |volume=267 |issue=7 |pages=1101–1108 |date=2009 |doi=10.1016/j.nimb.2009.01.132 |last2=Stansbery |first2=Eileen K. |last3=Keller |first3=Lindsay P. |bibcode=2009NIMPB.267.1101C |url=https://zenodo.org/record/1259269 |access-date=13 July 2019 |archive-date=11 May 2020 |archive-url=https://web.archive.org/web/20200511052700/https://zenodo.org/record/1259269 |url-status=live }}</ref>
]

]
== Observation by eyes ==
]
===Exposure to the eye===
]
] from the lenses. The eye also sees glare when looked towards the Sun directly.|left|alt=See caption]]
]

]
The brightness of the Sun can cause pain from looking at it with the ]; however, doing so for brief periods is not hazardous for normal non-] eyes.<ref>{{Cite journal |first1=T. J. |last1=White |first2=M. A. |last2=Mainster |first3=P. W. |last3=Wilson |first4=J. H. |last4=Tips |title=Chorioretinal temperature increases from solar observation |journal=] |volume=33 |issue=1 |pages=1–17 |year=1971 |doi=10.1007/BF02476660 |pmid=5551296}}</ref><ref>{{Cite journal |first1=M. O. M. |last1=Tso |first2=F. G. |last2=La Piana |title=The Human Fovea After Sungazing |journal=Transactions of the American Academy of Ophthalmology and Otolaryngology |year=1975 |volume=79 |pages=OP788–95 |pmid=1209815 |issue=6}}</ref> Looking directly at the Sun (]) causes ] visual artifacts and temporary partial blindness. It also delivers about 4&nbsp;milliwatts of sunlight to the retina, slightly heating it and potentially causing damage in eyes that cannot respond properly to the brightness.<ref>{{Cite journal |last1=Hope-Ross |first1=M. W. |title=Ultrastructural findings in solar retinopathy |journal=] |volume=7 |issue=4 |year=1993 |doi=10.1038/eye.1993.7 |pmid=8325420 |last2=Mahon |first2=G. J. |last3=Gardiner |first3=T. A. |last4=Archer |first4=D. B.|pages=29–33|doi-access=free }}</ref><ref>{{Cite journal |title=Solar Retinopathy from Sun-Gazing Under Influence of LSD |last1=Schatz |first1=H. |last2=Mendelblatt |first2=F. |journal=] |volume=57 |issue=4 |year=1973 |doi=10.1136/bjo.57.4.270 |pmid=4707624|pmc=1214879 |pages=270–273}}</ref> Viewing of the direct Sun with the naked eye can cause UV-induced, sunburn-like lesions on the retina beginning after about 100&nbsp;seconds, particularly under conditions where the UV light from the Sun is intense and well focused.<ref>{{Cite journal |first1=W. T. Jr. |last1=Ham |first2=H. A. |last2=Mueller |first3=D. H. |last3=Sliney |journal=] |title=Retinal sensitivity to damage from short wavelength light |volume=260 |issue=5547 |pages=153–155 |year=1976 |doi=10.1038/260153a0 |pmid=815821|bibcode=1976Natur.260..153H|s2cid=4283242 }}</ref><ref>{{Cite book |first1=W. T. Jr. |last1=Ham |first2=H. A. |last2=Mueller |first3=J. J. Jr. |last3=Ruffolo |first4=D. III |last4=Guerry |chapter=Solar Retinopathy as a function of Wavelength: its Significance for Protective Eyewear |title=The Effects of Constant Light on Visual Processes |editor-last=Williams |editor-first=T. P. |editor-last2=Baker |editor-first2=B. N. |publisher=] |pages=319–346 |year=1980 |isbn=978-0-306-40328-6}}</ref>
]

]
Viewing the Sun through light-concentrating ] such as ] may result in permanent damage to the retina without an appropriate filter that blocks UV and substantially dims the sunlight. When using an attenuating filter to view the Sun, the viewer is cautioned to use a filter specifically designed for that use. Some improvised filters that pass UV or ] rays, can actually harm the eye at high brightness levels.<ref>{{Cite book |first=T. |last=Kardos |title=Earth science |url=https://books.google.com/books?id=xI6EDV_PRr4C&pg=PT102 |page=87 |publisher=J. W. Walch |year=2003 |isbn=978-0-8251-4500-1 |access-date=22 August 2020}}</ref> Brief glances at the midday Sun through an unfiltered telescope can cause permanent damage.<ref name=Macdonald>{{cite book |last=Macdonald |first=Lee |chapter=Equipment for Observing the Sun |year=2012 |title=How to Observe the Sun Safely |publisher=Springer |place=New York |page=17 |doi=10.1007/978-1-4614-3825-0_2 |quote=Never look directly at the Sun through any form of optical equipment, even for an instant. A brief glimpse of the Sun through a telescope is enough to cause permanent eye damage, or even blindness. Even looking at the Sun with the naked eye for more than a second or two is not safe. Do not assume that it is safe to look at the Sun through a filter, no matter how dark the filter appears to be. |series=Patrick Moore's Practical Astronomy Series |isbn=978-1-4614-3824-3}}</ref>
]

]
During sunrise and sunset, sunlight is attenuated because of ] and ] from a particularly long passage through Earth's atmosphere,<ref name=Haber2005>{{Cite journal |last1=Haber |first1=Jorg |last2=Magnor |first2=Marcus |last3=Seidel |first3=Hans-Peter |title=Physically based Simulation of Twilight Phenomena |year=2005 |journal=ACM Transactions on Graphics |volume=24 |issue=4 |pages=1353–1373 |doi=10.1145/1095878.1095884 |citeseerx=10.1.1.67.2567 |s2cid=2349082}}</ref> and the Sun is sometimes faint enough to be viewed comfortably with the naked eye or safely with optics (provided there is no risk of bright sunlight suddenly appearing through a break between clouds). Hazy conditions, atmospheric dust, and high humidity contribute to this atmospheric attenuation.<ref>{{Cite journal |title=Diurnal asymmetries in global radiation |first=I. G. |last=Piggin |journal= Archiv für Meteorologie, Geophysik und Bioklimatologie, Serie B|year=1972 |volume=20 |issue=1 |doi=10.1007/BF02243313 |pages=41–48|bibcode=1972AMGBB..20...41P|s2cid=118819800 }}</ref>
]

]
===Phenomena===
]
An ], known as a ], can sometimes be seen shortly after sunset or before sunrise. The flash is caused by light from the Sun just below the horizon being ] (usually through a ]) towards the observer. Light of shorter wavelengths (violet, blue, green) is bent more than that of longer wavelengths (yellow, orange, red) but the violet and blue light is ] more, leaving light that is perceived as green.<ref>{{cite web |title=The Green Flash |url=https://www.bbc.co.uk/weather/features/understanding/greenflash.shtml | date=16 December 2008 |publisher=BBC |access-date=10 August 2008 |archive-url=https://web.archive.org/web/20081216135504/http://www.bbc.co.uk/weather/features/understanding/greenflash.shtml |archive-date=16 December 2008}}</ref>
]

]
== Religious aspects ==
]
{{Main|Solar deity}}
]
] by ancient Shu people. The center is a sun pattern with twelve points around which four ] fly in the same counterclockwise direction. ], coinciding with the ].|alt=See caption]]
]
Solar deities play a major role in many world religions and mythologies.<ref name="APLLondon">{{cite book |last1=Coleman |first1=J. A. |last2=Davidson |first2=George |title=The Dictionary of Mythology: An A–Z of Themes, Legends, and Heroes |year=2015 |publisher=Arcturus |location=London |isbn=978-1-78404-478-7 |page=316}}</ref> ] was central to civilizations such as the ]ians, the ] of South America and the ]s of what is now Mexico. In religions such as ], the Sun is still considered a god, known as ]. Many ancient monuments were constructed with solar phenomena in mind; for example, stone ]s accurately mark the summer or winter ] (for example in ], Egypt; ], Malta; and ], England); ], a prehistoric human-built mount in Ireland, was designed to detect the winter solstice; the pyramid of ] at ] in Mexico is designed to cast shadows in the shape of serpents climbing the ] at the vernal and autumnal ]es.<ref>{{cite journal|journal=]|title=El Sol en Chichén Itza y Dzibilchaltún. La Supuesta Importancia de los Equinoccios en Mesoamérica|language=es|first1=Ivan|last1=Šprajc|first2=Pedro Francisco Sanchéz|last2=Nava|date=21 March 2018 |number=149|pages=26–31|volume=XXV|url=https://arqueologiamexicana.mx/mexico-antiguo/el-sol-en-chichen-itza-y-dzibilchaltun-la-supuesta-importancia-de-los-equinoccios-en}}</ref>
]

]
The ancient ]ians believed that the Sun was ],<ref name=BlackGreen1992>{{cite book |last1=Black |first1=Jeremy |first2=Anthony |last2=Green |title=Gods, Demons and Symbols of Ancient Mesopotamia: An Illustrated Dictionary |url=https://books.google.com/books?id=05LXAAAAMAAJ&q=Inana |publisher=The British Museum Press |year=1992 |isbn=978-0-7141-1705-8 |pages=182–184 |access-date=22 August 2020}}</ref><ref name=Nemet1998>{{citation |last=Nemet-Nejat |first=Karen Rhea |year=1998 |title=Daily Life in Ancient Mesopotamia |publisher=Greenwood |isbn=978-0-313-29497-6 |page= |url=https://archive.org/details/dailylifeinancie00neme/page/203}}</ref> the god of justice and twin brother of ], the ],<ref name=BlackGreen1992 /> who was identified as the planet Venus.<ref name=Nemet1998 /> Later, Utu was identified with the ] god ].<ref name=BlackGreen1992 /><ref name=Nemet1998 /> Utu was regarded as a helper-deity, who aided those in distress.<ref name=BlackGreen1992 />
]
], 13th&nbsp;century&nbsp;BC|alt=A painting of Ra and Nefertari]]
]

]
From at least the ] of Ancient Egypt, the Sun was worshipped as the ], portrayed as a falcon-headed divinity surmounted by the solar disk, and surrounded by a serpent. In the ] period, the Sun became identified with the ]. In the form of the sun disc ], the Sun had a brief resurgence during the ] when it again became the preeminent, if not only, divinity for the Pharaoh ].<ref>{{cite book |last1=Teeter |first1=Emily |title=Religion and Ritual in Ancient Egypt |year=2011 |publisher=Cambridge University Press |location=New York |isbn=978-0-521-84855-8}}</ref><ref>{{cite book |last1=Frankfort |first1=Henri |title=Ancient Egyptian Religion: an Interpretation |year=2011 |publisher=Dover Publications |isbn=978-0-486-41138-5}}</ref> The Egyptians portrayed the god Ra as being carried across the sky in a solar barque, accompanied by lesser gods, and to the Greeks, he was Helios, carried by a chariot drawn by fiery horses. From the reign of ] in the ] the Sun's birthday was a holiday celebrated as ] (literally "Unconquered Sun") soon after the winter solstice, which may have been an antecedent to ]. Regarding the ]s, the Sun appears from Earth to revolve once a year along the ] through the ], and so Greek astronomers categorized it as one of the seven ] (Greek ''planetes'', "wanderer"); the naming of the ] after the seven planets dates to the ].<ref name="oed">{{cite web |url=http://www.oxforddictionaries.com/definition/american_english/planet |publisher=Oxford Dictionaries |title=Planet |access-date=22 March 2015 |date=December 2007 |archive-date=2 April 2015 |archive-url=https://web.archive.org/web/20150402154243/http://www.oxforddictionaries.com/definition/american_english/planet |url-status=dead }}</ref><ref name="almagest">{{Cite journal |first=Bernard R. |last=Goldstein |title=Saving the phenomena : the background to Ptolemy's planetary theory |journal=Journal for the History of Astronomy |volume=28 |issue=1 |year=1997 |pages=1–12 |bibcode=1997JHA....28....1G|doi=10.1177/002182869702800101|s2cid=118875902 }}</ref><ref>{{Cite book |title=Ptolemy's Almagest |author=Ptolemy |last2=Toomer |first2=G.J. |publisher=Princeton University Press |year=1998 |isbn=978-0-691-00260-6}}</ref>
]

]
In ], the Sun was personified as the goddess ].<ref>{{cite encyclopedia |year=1997 |title=Encyclopedia of Indo-European Culture |editor1-last=Mallory |editor1-first=James P. |editor1-link=J. P. Mallory |editor2-last=Adams |editor2-first=Douglas Q. |editor2-link=Douglas Q. Adams |place=London |publisher=Routledge |id=(EIEC) |url=https://books.google.com/books?id=tzU3RIV2BWIC&q=Sun+goddess |isbn=978-1-884964-98-5 |access-date=20 October 2017}}</ref><ref name=MALLORY129>{{cite book |last=Mallory |first=J. P. |year=1989 |title=In Search of the Indo-Europeans: Language, Archaeology and Myth |url=https://archive.org/details/insearchofindoeu00jpma |url-access=registration |page= |publisher=] |isbn=978-0-500-27616-7}}</ref> Derivatives of this goddess in ] include the ] '']'', ] '']'', ] '']'', ] '']'', and ] ''Solntse''.<ref name=MALLORY129 /> In ], the sun deity was the male god Helios,<ref>{{cite web | title=Hesiod, ''Theogony'' line 371 | work=Perseus Digital Library | url=https://www.perseus.tufts.edu/hopper/text?doc=Perseus%3Atext%3A1999.01.0130%3Acard%3D371 | access-date=2024-05-28 | archive-url=https://web.archive.org/web/20210915222218/https://www.perseus.tufts.edu/hopper/text?doc=Perseus:text:1999.01.0130:card%3D371 |date=15 September 2021 | archive-date=2021-09-15 }}</ref> who in later times was ] with ].<ref>{{cite book |last=Burkert |first=Walter |author-link=Walter Burkert |year=1985 |title=Greek Religion |publisher=Harvard University Press |location=Cambridge |isbn=978-0-674-36281-9 |page=120}}</ref>
]

]
In the ], Malachi 4:2 mentions the "Sun of Righteousness" (sometimes translated as the "Sun of Justice"),<ref>{{Bibleverse||Malachi|4:2|9}}</ref><ref>{{citation |title=Bible, Book of Malachi |publisher=King James Version |url=https://www.biblegateway.com/passage/?search=Malachi+4&version=KJV |access-date=20 October 2017 |archive-date=20 October 2017 |archive-url=https://web.archive.org/web/20171020140215/https://www.biblegateway.com/passage/?search=Malachi+4&version=KJV |url-status=live }}</ref> which some ] have interpreted as a reference to the ] (]).<ref>{{cite book |last=Spargo |first=Emma Jane Marie |title=The Category of the Aesthetic in the Philosophy of Saint Bonaventure |url=https://books.google.com/books?id=SUkWAAAAMAAJ&q=sol+iustitiae+malachiae+IV+2&pg=PA86 |page=86 |year=1953 |publisher=The Franciscan Institute |location=St. Bonaventure, New York; E. Nauwelaerts, Louvain, Belgium; F. Schöningh, Paderborn, Germany}}</ref> In ancient Roman culture, ] was the day of the sun god. In paganism, the Sun was a source of life, giving warmth and illumination. It was the center of a popular cult among Romans, who would stand at dawn to catch the first rays of sunshine as they prayed. The celebration of the ] (which influenced Christmas) was part of the Roman cult of the unconquered Sun (]). It was adopted as the ] day by Christians. The symbol of light was a pagan device adopted by Christians, and perhaps the most important one that did not come from Jewish traditions. Christian churches were built so that the congregation faced toward the sunrise.<ref>{{cite book | first=Owen | last=Chadwick |title=A History of Christianity |url=https://books.google.com/books?id=qugouOh3KjMC&pg=PA22 |year=1998 |publisher=St. Martin's |page=22 |isbn=978-0-312-18723-1 |access-date=15 November 2015}}</ref>
]

]
], the Aztec god of the sun,<ref name=Townsend1979>{{cite book |title=State and Cosmos in the Art of Tenochtitlan |url=https://archive.org/details/statecosmosinart00town | access-date=2024-05-28 |url-access=registration |last=Townsend |first=Richard |publisher=Dumbarton Oaks |year=1979 |location=Washington, DC |page=}}</ref> was closely associated with the practice of ].<ref name=Townsend1979 /> The sun goddess ] is the most important deity in the ] religion,<ref name="Roberts 110">{{cite book |last=Roberts |first=Jeremy |title=Japanese Mythology A To Z |location=New York |publisher=] |year=2010 |edition=2nd |isbn=978-1-60413-435-3 |pages=4–5}}</ref><ref>{{cite book |last=Wheeler |first=Post |title=The Sacred Scriptures of the Japanese |location=New York |publisher=Henry Schuman |pages=393–395 |year=1952 |isbn=978-1-4254-8787-4}}</ref> and she is believed to be the direct ancestor of all ].<ref name="Roberts 110" />
]

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== See also ==
]
{{Portal|Astronomy|Stars|Solar System|Weather|Physics}}
]
{{div col|colwidth=30em}}
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* {{Annotated link |Advanced Composition Explorer}}
]
* {{Annotated link |Analemma}}
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* {{Annotated link |Antisolar point}}
]
* {{Annotated link |Faint young Sun paradox}}
]
* {{Annotated link |List of brightest stars}}
]
* {{Annotated link |List of nearest stars}}
]
* {{Annotated link |Midnight sun}}
]
* {{slink|Planets in astrology|Sun}}
]
* {{Annotated link |Solar telescope}}
]
* {{Annotated link |Sun path}}
]
* {{Annotated link |Sun-Earth Day}}
]
* {{Annotated link|The Sun in culture}}
]
* ]
]
* {{Annotated link |Timeline of the far future}}
]
{{div col end}}
]

]
== Notes ==
]
{{reflist|group=note}}
]
{{notelist
]
| notes =
]
{{efn
]
| name = heavy elements
]
| In ], the term ''heavy elements'' (or ''metals'') refers to all chemical elements except hydrogen and helium.
]
}}
]
{{efn
| name = particle density
| Earth's atmosphere near sea level has a particle density of about 2{{e|25}}&nbsp;m<sup>−3</sup>.
}}
{{efn
| name=rotation
| Counterclockwise is also the direction of revolution around the Sun for objects in the Solar System and is the direction of axial spin for most objects.
}}
}}

== References ==
{{reflist}}

== Further reading ==
{{Library resources box
|by=no
|onlinebooksabout=yes
|others=
|about=yes
|label=Sun
|viaf= |lccn= |lcheading=Sun |wikititle=
}}
* {{Cite book |last=Cohen |first=Richard |url=https://books.google.com/books?id=rspEEVTcmIAC |title=Chasing the sun: the epic story of the star that gives us life |publisher=Random House |year=2010 |isbn=978-1-4000-6875-3 |location=New York, NY}}
* {{Cite encyclopedia |title=Solar activity |encyclopedia=] |url=http://www.scholarpedia.org/article/Solar_activity |last=Hudson |first=Hugh |date=2008 |volume=3 |issue=3 |page=3967 |bibcode=2008SchpJ...3.3967H |doi=10.4249/scholarpedia.3967 |issn=1941-6016 |doi-access=free}}
* {{Cite journal |last=Thompson |first=Michael J |date=August 2004 |title=Helioseismology and the Sun's interior |journal=] |volume=45 |issue=4 |pages=4.21–4.25 |bibcode=2004A&G....45d..21T |doi=10.1046/j.1468-4004.2003.45421.x |issn=1366-8781 |doi-access=free}}

== External links ==
{{Spoken Misplaced Pages|date=2021-06-07|En-Sun.ogg}}
{{Sister project links|Sun|v=no|n=no|b=no|s=no}}
*
* {{Webarchive|url=https://web.archive.org/web/20170611210135/http://acrim.com/ |date=11 June 2017 }}
*
* | ]
* | Goddard Space Flight Center

{{The Sun|state=uncollapsed}}
{{Sun spacecraft}}
{{Solar System}}
{{Star}}
{{Nearest star systems|1}}
{{Astronomy navbar}}
{{Authority control}}

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Latest revision as of 03:08, 1 January 2025

Star at the center of the Solar System "The Sun" redirects here. For other uses, see Sun (disambiguation) and The Sun (disambiguation).

Sun
White glowing ball with black sunspotsThe Sun, viewed through a clear solar filter
NamesSun, Sol, Sól, Helios
AdjectivesSolar
SymbolCircle with dot in the middle
Observation data
Mean distance from EarthAU
149,600,000 km
8 min 19 s, light speed
Visual brightness−26.74 (V)
Absolute magnitude4.83
Spectral classificationG2V
MetallicityZ = 0.0122
Angular size0.527–0.545°
Orbital characteristics
Mean distance from Milky Way core24,000 to 28,000 light-years
Galactic period225–250 million years
Velocity
Obliquity
Right ascension North pole286.13° (286° 7′ 48″)
Declination of North pole+63.87° (63° 52′ 12"N)
Sidereal rotation period
  • 25.05 days (equator)
  • 34.4 days (poles)
Equatorial rotation velocity1.997 km/s
Physical characteristics
Equatorial radius6.957×10 m
109 × Earth radii
Flattening0.00005
Surface area6.09×10 km
12,000 × Earth
Volume
  • 1.412×10 km
  • 1,300,000 × Earth
Mass
Average density1.408 g/cm
0.255 × Earth
Age4.6 billion years
Equatorial surface gravity274 m/s
27.9 g0
Moment of inertia factor≈0.070
Surface escape velocity617.7 km/s
55 × Earth
Temperature
Luminosity
Color (B-V)0.656
Mean radiance2.009×10 W·m·sr
Photosphere composition by mass

The Sun is the star at the center of the Solar System. It is a massive, nearly perfect sphere of hot plasma, heated to incandescence by nuclear fusion reactions in its core, radiating the energy from its surface mainly as visible light and infrared radiation with 10% at ultraviolet energies. It is by far the most important source of energy for life on Earth. The Sun has been an object of veneration in many cultures. It has been a central subject for astronomical research since antiquity.

The Sun orbits the Galactic Center at a distance of 24,000 to 28,000 light-years. From Earth, it is 1 astronomical unit (1.496×10 km) or about 8 light-minutes away. Its diameter is about 1,391,400 km (864,600 mi), 109 times that of Earth. Its mass is about 330,000 times that of Earth, making up about 99.86% of the total mass of the Solar System. Roughly three-quarters of the Sun's mass consists of hydrogen (~73%); the rest is mostly helium (~25%), with much smaller quantities of heavier elements, including oxygen, carbon, neon, and iron.

The Sun is a G-type main-sequence star (G2V), informally called a yellow dwarf, though its light is actually white. It formed approximately 4.6 billion years ago from the gravitational collapse of matter within a region of a large molecular cloud. Most of this matter gathered in the center, whereas the rest flattened into an orbiting disk that became the Solar System. The central mass became so hot and dense that it eventually initiated nuclear fusion in its core. Every second, the Sun's core fuses about 600 billion kilograms (kg) of hydrogen into helium and converts 4 billion kg of matter into energy.

About 4 to 7 billion years from now, when hydrogen fusion in the Sun's core diminishes to the point where the Sun is no longer in hydrostatic equilibrium, its core will undergo a marked increase in density and temperature which will cause its outer layers to expand, eventually transforming the Sun into a red giant. This process will make the Sun large enough to render Earth uninhabitable approximately five billion years from the present. After the red giant phase, models suggest the Sun will shed its outer layers and become a dense type of cooling star (a white dwarf), and no longer produce energy by fusion, but will still glow and give off heat from its previous fusion for perhaps trillions of years. After that, it is theorized to become a super dense black dwarf, giving off negligible energy.

Etymology

The English word sun developed from Old English sunne. Cognates appear in other Germanic languages, including West Frisian sinne, Dutch zon, Low German Sünn, Standard German Sonne, Bavarian Sunna, Old Norse sunna, and Gothic sunnō. All these words stem from Proto-Germanic *sunnōn. This is ultimately related to the word for sun in other branches of the Indo-European language family, though in most cases a nominative stem with an l is found, rather than the genitive stem in n, as for example in Latin sōl, ancient Greek ἥλιος (hēlios), Welsh haul and Czech slunce, as well as (with *l > r) Sanskrit स्वर् (svár) and Persian خور (xvar). Indeed, the l-stem survived in Proto-Germanic as well, as *sōwelan, which gave rise to Gothic sauil (alongside sunnō) and Old Norse prosaic sól (alongside poetic sunna), and through it the words for sun in the modern Scandinavian languages: Swedish and Danish sol, Icelandic sól, etc.

The principal adjectives for the Sun in English are sunny for sunlight and, in technical contexts, solar (/ˈsoʊlər/), from Latin sol. From the Greek helios comes the rare adjective heliac (/ˈhiːliæk/). In English, the Greek and Latin words occur in poetry as personifications of the Sun, Helios (/ˈhiːliəs/) and Sol (/ˈsɒl/), while in science fiction Sol may be used to distinguish the Sun from other stars. The term sol with a lowercase s is used by planetary astronomers for the duration of a solar day on another planet such as Mars.

The astronomical symbol for the Sun is a circle with a center dot, ☉. It is used for such units as M (Solar mass), R (Solar radius) and L (Solar luminosity). The scientific study of the Sun is called heliology.

General characteristics

Size comparison of the Sun, all the planets of the Solar System and some larger stars. The Sun is 1.4 million kilometers (4.643 light-seconds) wide, about 109 times wider than Earth, or four times the Lunar distance, and contains 99.86% of all Solar System mass.

The Sun is a G-type main-sequence star that makes up about 99.86% of the mass of the Solar System. It has an absolute magnitude of +4.83, estimated to be brighter than about 85% of the stars in the Milky Way, most of which are red dwarfs. It is more massive than 95% of the stars within 7 pc (23 ly). The Sun is a Population I, or heavy-element-rich, star. Its formation approximately 4.6 billion years ago may have been triggered by shockwaves from one or more nearby supernovae. This is suggested by a high abundance of heavy elements in the Solar System, such as gold and uranium, relative to the abundances of these elements in so-called Population II, heavy-element-poor, stars. The heavy elements could most plausibly have been produced by endothermic nuclear reactions during a supernova, or by transmutation through neutron absorption within a massive second-generation star.

The Sun is by far the brightest object in the Earth's sky, with an apparent magnitude of −26.74. This is about 13 billion times brighter than the next brightest star, Sirius, which has an apparent magnitude of −1.46.

One astronomical unit (about 150 million kilometres; 93 million miles) is defined as the mean distance between the centers of the Sun and the Earth. The instantaneous distance varies by about ±2.5 million kilometres (1.6 million miles) as Earth moves from perihelion around 3 January to aphelion around 4 July. At its average distance, light travels from the Sun's horizon to Earth's horizon in about 8 minutes and 20 seconds, while light from the closest points of the Sun and Earth takes about two seconds less. The energy of this sunlight supports almost all life on Earth by photosynthesis, and drives Earth's climate and weather.

The Sun does not have a definite boundary, but its density decreases exponentially with increasing height above the photosphere. For the purpose of measurement, the Sun's radius is considered to be the distance from its center to the edge of the photosphere, the apparent visible surface of the Sun. The roundness of the Sun is relative difference between its radius at its equator, R eq {\displaystyle R_{\textrm {eq}}} , and at its pole, R pol {\displaystyle R_{\textrm {pol}}} , called the oblateness, Δ = ( R eq R pol ) / R pol . {\displaystyle \Delta _{\odot }=(R_{\textrm {eq}}-R_{\textrm {pol}})/R_{\textrm {pol}}.} The value is difficult to measure. Atmospheric distortion means the measurement must be done on satellites; the value is very small meaning very precise technique is needed.

The oblateness was once proposed to be sufficient to explain the perihelion precession of Mercury but Einstein proposed that general relativity could explain the precession using a spherical Sun. When high precision measurements of the oblateness became available via the Solar Dynamics Observatory and the Picard satellite the measured value was even smaller than expected, 8.2 x 10, or 8 parts per million. This makes the Sun the natural object closest to a perfect sphere. The oblateness value remains constant independent of solar irradiation changes. The tidal effect of the planets is weak and does not significantly affect the shape of the Sun.

Rotation

Main article: Solar rotation

The Sun rotates faster at its equator than at its poles. This differential rotation is caused by convective motion due to heat transport and the Coriolis force due to the Sun's rotation. In a frame of reference defined by the stars, the rotational period is approximately 25.6 days at the equator and 33.5 days at the poles. Viewed from Earth as it orbits the Sun, the apparent rotational period of the Sun at its equator is about 28 days. Viewed from a vantage point above its north pole, the Sun rotates counterclockwise around its axis of spin.

A survey of solar analogs suggest the early Sun was rotating up to ten times faster than it does today. This would have made the surface much more active, with greater X-ray and UV emission. Sun spots would have covered 5–30% of the surface. The rotation rate was gradually slowed by magnetic braking, as the Sun's magnetic field interacted with the outflowing solar wind. A vestige of this rapid primordial rotation still survives at the Sun's core, which has been found to be rotating at a rate of once per week; four times the mean surface rotation rate.

Composition

See also: Molecules in stars

The Sun consists mainly of the elements hydrogen and helium. At this time in the Sun's life, they account for 74.9% and 23.8%, respectively, of the mass of the Sun in the photosphere. All heavier elements, called metals in astronomy, account for less than 2% of the mass, with oxygen (roughly 1% of the Sun's mass), carbon (0.3%), neon (0.2%), and iron (0.2%) being the most abundant.

The Sun's original chemical composition was inherited from the interstellar medium out of which it formed. Originally it would have been about 71.1% hydrogen, 27.4% helium, and 1.5% heavier elements. The hydrogen and most of the helium in the Sun would have been produced by Big Bang nucleosynthesis in the first 20 minutes of the universe, and the heavier elements were produced by previous generations of stars before the Sun was formed, and spread into the interstellar medium during the final stages of stellar life and by events such as supernovae.

Since the Sun formed, the main fusion process has involved fusing hydrogen into helium. Over the past 4.6 billion years, the amount of helium and its location within the Sun has gradually changed. The proportion of helium within the core has increased from about 24% to about 60% due to fusion, and some of the helium and heavy elements have settled from the photosphere toward the center of the Sun because of gravity. The proportions of heavier elements are unchanged. Heat is transferred outward from the Sun's core by radiation rather than by convection (see Radiative zone below), so the fusion products are not lifted outward by heat; they remain in the core, and gradually an inner core of helium has begun to form that cannot be fused because presently the Sun's core is not hot or dense enough to fuse helium. In the current photosphere, the helium fraction is reduced, and the metallicity is only 84% of what it was in the protostellar phase (before nuclear fusion in the core started). In the future, helium will continue to accumulate in the core, and in about 5 billion years this gradual build-up will eventually cause the Sun to exit the main sequence and become a red giant.

The chemical composition of the photosphere is normally considered representative of the composition of the primordial Solar System. Typically, the solar heavy-element abundances described above are measured both by using spectroscopy of the Sun's photosphere and by measuring abundances in meteorites that have never been heated to melting temperatures. These meteorites are thought to retain the composition of the protostellar Sun and are thus not affected by the settling of heavy elements. The two methods generally agree well.

Structure and fusion

Main article: Standard solar model
See caption
Illustration of the Sun's structure, in false color for contrast

Core

Main article: Solar core

The core of the Sun extends from the center to about 20–25% of the solar radius. It has a density of up to 150 g/cm (about 150 times the density of water) and a temperature of close to 15.7 million kelvin (K). By contrast, the Sun's surface temperature is about 5800 K. Recent analysis of SOHO mission data favors the idea that the core is rotating faster than the radiative zone outside it. Through most of the Sun's life, energy has been produced by nuclear fusion in the core region through the proton–proton chain; this process converts hydrogen into helium. Currently, 0.8% of the energy generated in the Sun comes from another sequence of fusion reactions called the CNO cycle; the proportion coming from the CNO cycle is expected to increase as the Sun becomes older and more luminous.

The core is the only region of the Sun that produces an appreciable amount of thermal energy through fusion; 99% of the Sun's power is generated in the innermost 24% of its radius, and almost no fusion occurs beyond 30% of the radius. The rest of the Sun is heated by this energy as it is transferred outward through many successive layers, finally to the solar photosphere where it escapes into space through radiation (photons) or advection (massive particles).

circles and arrows showing protons combining in a series of fusion reactions yielding helium-3 which breaks down tow helium-4
Illustration of a proton-proton reaction chain, from hydrogen forming deuterium, helium-3, and regular helium-4

The proton–proton chain occurs around 9.2×10 times each second in the core, converting about 3.7×10 protons into alpha particles (helium nuclei) every second (out of a total of ~8.9×10 free protons in the Sun), or about 6.2×10 kg/s. However, each proton (on average) takes around 9 billion years to fuse with another using the PP chain. Fusing four free protons (hydrogen nuclei) into a single alpha particle (helium nucleus) releases around 0.7% of the fused mass as energy, so the Sun releases energy at the mass–energy conversion rate of 4.26 billion kg/s (which requires 600 billion kg of hydrogen), for 384.6 yottawatts (3.846×10 W), or 9.192×10 megatons of TNT per second. The large power output of the Sun is mainly due to the huge size and density of its core (compared to Earth and objects on Earth), with only a fairly small amount of power being generated per cubic metre. Theoretical models of the Sun's interior indicate a maximum power density, or energy production, of approximately 276.5 watts per cubic metre at the center of the core, which, according to Karl Kruszelnicki, is about the same power density inside a compost pile.

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 density and hence the fusion rate and correcting the perturbation; and a slightly lower rate would cause the core to cool and shrink slightly, increasing the density and increasing the fusion rate and again reverting it to its present rate.

Radiative zone

Main article: Radiative zone
See caption
Illustration of different stars' internal structure based on mass. The Sun in the middle has an inner radiating zone and an outer convective zone.

The radiative zone is the thickest layer of the Sun, at 0.45 solar radii. From the core out to about 0.7 solar radii, thermal radiation is the primary means of energy transfer. The temperature drops from approximately 7 million to 2 million kelvins with increasing distance from the core. This temperature gradient is less than the value of the adiabatic lapse rate and hence cannot drive convection, which explains why the transfer of energy through this zone is by radiation instead of thermal convection. Ions of hydrogen and helium emit photons, which travel only a brief distance before being reabsorbed by other ions. The density drops a hundredfold (from 20,000 kg/m to 200 kg/m) between 0.25 solar radii and 0.7 radii, the top of the radiative zone.

Tachocline

Main article: Tachocline

The radiative zone and the convective zone are separated by a transition layer, the tachocline. This is a region where the sharp regime change between the uniform rotation of the radiative zone and the differential rotation of the convection zone results in a large shear between the two—a condition where successive horizontal layers slide past one another. Presently, it is hypothesized that a magnetic dynamo, or solar dynamo, within this layer generates the Sun's magnetic field.

Convective zone

Main article: Convection zone

The Sun's convection zone extends from 0.7 solar radii (500,000 km) to near the surface. In this layer, the solar plasma is not dense or hot enough to transfer the heat energy of the interior outward via radiation. Instead, the density of the plasma is low enough to allow convective currents to develop and move the Sun's energy outward towards its surface. Material heated at the tachocline picks up heat and expands, thereby reducing its density and allowing it to rise. As a result, an orderly motion of the mass develops into thermal cells that carry most of the heat outward to the Sun's photosphere above. Once the material diffusively and radiatively cools just beneath the photospheric surface, its density increases, and it sinks to the base of the convection zone, where it again picks up heat from the top of the radiative zone and the convective cycle continues. At the photosphere, the temperature has dropped 350-fold to 5,700 K (9,800 °F) and the density to only 0.2 g/m (about 1/10,000 the density of air at sea level, and 1 millionth that of the inner layer of the convective zone).

The thermal columns of the convection zone form an imprint on the surface of the Sun giving it a granular appearance called the solar granulation at the smallest scale and supergranulation at larger scales. Turbulent convection in this outer part of the solar interior sustains "small-scale" dynamo action over the near-surface volume of the Sun. The Sun's thermal columns are Bénard cells and take the shape of roughly hexagonal prisms.

Photosphere

Main article: Photosphere
A miasma of plasma
Image of the Sun's cell-like surface structures

The visible surface of the Sun, the photosphere, is the layer below which the Sun becomes opaque to visible light. Photons produced in this layer escape the Sun through the transparent solar atmosphere above it and become solar radiation, sunlight. The change in opacity is due to the decreasing amount of H ions, which absorb visible light easily. Conversely, the visible light perceived is produced as electrons react with hydrogen atoms to produce H ions.

The photosphere is tens to hundreds of kilometers thick, and is 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. The spectrum of sunlight has approximately the spectrum of a black-body radiating at 5,772 K (9,930 °F), interspersed with atomic absorption lines from the tenuous layers above the photosphere. The photosphere has a particle density of ~10 m (about 0.37% of the particle number per volume of Earth's atmosphere at sea level). The photosphere is not fully ionized—the extent of ionization is about 3%, leaving almost all of the hydrogen in atomic form.

Atmosphere

Main article: Stellar atmosphere

The Sun's atmosphere is composed of five layers: the photosphere, the chromosphere, the transition region, the corona, and the heliosphere.

The coolest layer of the Sun is a temperature minimum region extending to about 500 km above the photosphere, and has a temperature of about 4,100 K. This part of the Sun is cool enough to allow for the existence of simple molecules such as carbon monoxide and water. The chromosphere, transition region, and corona are much hotter than the surface of the Sun. The reason is not well understood, but evidence suggests that Alfvén waves may have enough energy to heat the corona.

A photograph of the surface of the sun, with flares terminating from the surface on the left.
The Sun's transition region taken by Hinode's Solar Optical Telescope

Above the temperature minimum layer is a 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 solar eclipses. The temperature of the chromosphere increases gradually with altitude, ranging up to around 20,000 K near the top. In the upper part of the chromosphere helium becomes partially ionized.

Above the chromosphere, in a thin (about 200 km) transition region, the temperature rises rapidly from around 20,000 K in the upper chromosphere to coronal temperatures closer to 1,000,000 K. The temperature increase is facilitated by the full ionization of helium in the transition region, which significantly reduces radiative cooling of the plasma. The transition region does not occur at a well-defined altitude, but forms a kind of nimbus around chromospheric features such as spicules and filaments, and is in constant, chaotic motion. The transition region is not easily visible from Earth's surface, but is readily observable from space by instruments sensitive to extreme ultraviolet.

A photograph of a solar eclipse
During a solar eclipse the solar corona can be seen with the naked eye during totality.

The corona is the next layer of the Sun. The low corona, near the surface of the Sun, has a particle density around 10 m to 10 m. The average temperature of the corona and solar wind is about 1,000,000–2,000,000 K; however, in the hottest regions it is 8,000,000–20,000,000 K. Although no complete theory yet exists to account for the temperature of the corona, at least some of its heat is known to be from magnetic reconnection. The corona is the extended atmosphere of the Sun, which has a volume much larger than the volume enclosed by the Sun's photosphere. A flow of plasma outward from the Sun into interplanetary space is the solar wind.

The heliosphere, the tenuous outermost atmosphere of the Sun, is filled with solar wind plasma and is defined to begin at the distance where the flow of the solar wind becomes superalfvénic—that is, where the flow becomes faster than the speed of Alfvén waves, at approximately 20 solar radii (0.1 AU). Turbulence and dynamic forces in the heliosphere cannot affect the shape of the solar corona within, because the information can only travel at the speed of Alfvén waves. The solar wind travels outward continuously through the heliosphere, forming the solar magnetic field into a spiral shape, until it impacts the heliopause more than 50 AU from the Sun. In December 2004, the Voyager 1 probe passed through a shock front that is thought to be part of the heliopause. In late 2012, Voyager 1 recorded a marked increase in cosmic ray collisions and a sharp drop in lower energy particles from the solar wind, which suggested that the probe had passed through the heliopause and entered the interstellar medium, and indeed did so on August 25, 2012, at approximately 122 astronomical units (18 Tm) from the Sun. The heliosphere has a heliotail which stretches out behind it due to the Sun's peculiar motion through the galaxy.

On April 28, 2021, NASA's Parker Solar Probe encountered the specific magnetic and particle conditions at 18.8 solar radii that indicated that it penetrated the Alfvén surface, the boundary separating the corona from the solar wind, defined as where the coronal plasma's Alfvén speed and the large-scale solar wind speed are equal. During the flyby, Parker Solar Probe passed into and out of the corona several times. This proved the predictions that the Alfvén critical surface is not shaped like a smooth ball, but has spikes and valleys that wrinkle its surface.

Depiction of the heliosphere

Solar radiation

Main articles: Sunlight and Solar irradiance
A photograph of the sun with a layer of fog visible in front of it.
The Sun seen through a light fog

The Sun emits light across the visible spectrum, so its color is white, with a CIE color-space index near (0.3, 0.3), when viewed from space or when the Sun is high in the sky. The Solar radiance per wavelength peaks in the green portion of the spectrum when viewed from space. When the Sun is very low in the sky, atmospheric scattering renders the Sun yellow, red, orange, or magenta, and in rare occasions even green or blue. Some cultures mentally picture the Sun as yellow and some even red; the cultural reasons for this are debated. The Sun is classed as a G2 star, meaning it is a G-type star, with 2 indicating its surface temperature is in the second range of the G class.

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 1,368 W/m (watts per square meter) at a distance of one astronomical unit (AU) from the Sun (that is, at or near Earth's orbit). Sunlight on the surface of Earth is attenuated by Earth's atmosphere, so that less power arrives at the surface (closer to 1,000 W/m) in clear conditions when the Sun is near the zenith. Sunlight at the top of Earth's atmosphere is composed (by total energy) of about 50% infrared light, 40% visible light, and 10% ultraviolet light. The atmosphere filters out over 70% of solar ultraviolet, especially at the shorter wavelengths. Solar ultraviolet radiation ionizes Earth's dayside upper atmosphere, creating the electrically conducting ionosphere.

Ultraviolet light from the Sun has antiseptic properties and can be used to sanitize tools and water. This radiation causes sunburn, and has other biological effects such as the production of vitamin D and sun tanning. It is the main cause of skin cancer. Ultraviolet light is strongly attenuated by Earth's ozone layer, so that the amount of UV varies greatly with latitude and has been partially responsible for many biological adaptations, including variations in human skin color.

High-energy gamma ray photons initially released with fusion reactions in the core are almost immediately absorbed by the solar plasma of the radiative zone, usually after traveling only a few millimeters. Re-emission happens in a random direction and usually at slightly lower energy. With this sequence of emissions and absorptions, it takes a long time for radiation to reach the Sun's surface. Estimates of the photon travel time range between 10,000 and 170,000 years. In contrast, it takes only 2.3 seconds for neutrinos, which account for about 2% of the total energy production of the Sun, to reach the surface. Because energy transport in the Sun is a process that involves photons in thermodynamic equilibrium with matter, the time scale of energy transport in the Sun is longer, on the order of 30,000,000 years. This is the time it would take the Sun to return to a stable state if the rate of energy generation in its core were suddenly changed.

Electron neutrinos are released by fusion reactions in the core, but, unlike photons, they rarely interact with matter, so almost all are able to escape the Sun immediately. However, measurements of the number of these neutrinos produced in the Sun are lower than theories predict by a factor of 3. In 2001, the discovery of neutrino oscillation resolved the discrepancy: the Sun emits the number of electron neutrinos predicted by the theory, but neutrino detectors were missing 2⁄3 of them because the neutrinos had changed flavor by the time they were detected.

Magnetic activity

The Sun has a stellar magnetic field that varies across its surface. Its polar field is 1–2 gauss (0.0001–0.0002 T), whereas the field is typically 3,000 gauss (0.3 T) in features on the Sun called sunspots and 10–100 gauss (0.001–0.01 T) in solar prominences. The magnetic field varies in time and location. The quasi-periodic 11-year solar cycle is the most prominent variation in which the number and size of sunspots waxes and wanes.

The solar magnetic field extends well beyond the Sun itself. The electrically conducting solar wind plasma carries the Sun's magnetic field into space, forming what is called the interplanetary magnetic field. In an approximation known as ideal magnetohydrodynamics, plasma particles only move along magnetic field lines. As a result, the outward-flowing solar wind stretches the interplanetary magnetic field outward, forcing it into a roughly radial structure. For a simple dipolar solar magnetic field, with opposite hemispherical polarities on either side of the solar magnetic equator, a thin current sheet is formed in the solar wind. At great distances, the rotation of the Sun twists the dipolar magnetic field and corresponding current sheet into an Archimedean spiral structure called the Parker spiral.

Sunspot

Main article: Sunspot
A black-and-white photograph of a group of sunspots.
A large sunspot group observed in white light

Sunspots are visible as dark patches on the Sun's photosphere and correspond to concentrations of magnetic field where convective transport of heat is inhibited from the solar interior to the surface. As a result, sunspots are slightly cooler than the surrounding photosphere, so they appear dark. At a typical solar minimum, few sunspots are visible, and occasionally none can be seen at all. Those that do appear are at high solar latitudes. As the solar cycle progresses toward its maximum, sunspots tend to form closer to the solar equator, a phenomenon known as Spörer's law. The largest sunspots can be tens of thousands of kilometers across.

An 11-year sunspot cycle is half of a 22-year Babcock–Leighton dynamo cycle, which corresponds to an oscillatory exchange of energy between toroidal and poloidal solar magnetic fields. At solar-cycle maximum, the external poloidal dipolar magnetic field is near its dynamo-cycle minimum strength; but an internal toroidal quadrupolar field, generated through differential rotation within the tachocline, is near its maximum strength. At this point in the dynamo cycle, buoyant upwelling within the convective zone forces emergence of the toroidal magnetic field through the photosphere, giving rise to pairs of sunspots, roughly aligned east–west and having footprints with opposite magnetic polarities. The magnetic polarity of sunspot pairs alternates every solar cycle, a phenomenon described by Hale's law.

During the solar cycle's declining phase, energy shifts from the internal toroidal magnetic field to the external poloidal field, and sunspots diminish in number and size. At solar-cycle minimum, the toroidal field is, correspondingly, at minimum strength, sunspots are relatively rare, and the poloidal field is at its maximum strength. With the rise of the next 11-year sunspot cycle, differential rotation shifts magnetic energy back from the poloidal to the toroidal field, but with a polarity that is opposite to the previous cycle. The process carries on continuously, and in an idealized, simplified scenario, each 11-year sunspot cycle corresponds to a change, then, in the overall polarity of the Sun's large-scale magnetic field.

Solar activity

Main article: Solar cycle
See caption
Measurements from 2005 of solar cycle variation during the previous 30 years

The Sun's magnetic field leads to many effects that are collectively called solar activity. Solar flares and coronal mass ejections tend to occur at sunspot groups. Slowly changing high-speed streams of solar wind are emitted from coronal holes at the photospheric surface. Both coronal mass ejections and high-speed streams of solar wind carry plasma and the interplanetary magnetic field outward into the Solar System. The 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.

Long-term secular change in sunspot number is thought, by some scientists, to be correlated with long-term change in solar irradiance, which, in turn, might influence Earth's long-term climate. The solar cycle influences space weather conditions, including those surrounding Earth. For example, in the 17th century, the solar cycle appeared to have stopped entirely for several decades; few sunspots were observed during a period known as the Maunder minimum. This coincided in time with the era of the Little Ice Age, when Europe experienced unusually cold temperatures. Earlier extended minima have been discovered through analysis of tree rings and appear to have coincided with lower-than-average global temperatures.

Coronal heating

Main article: Stellar corona Unsolved problem in astronomy: Why is the Sun's corona so much hotter than the Sun's surface? (more unsolved problems in astronomy)

The temperature of the photosphere is approximately 6,000 K, whereas the temperature of the corona reaches 1,000,000–2,000,000 K. The high temperature of the corona shows that it is heated by something other than direct heat conduction from the photosphere.

It is thought that the energy necessary to heat the corona is provided by turbulent motion in the convection zone below the photosphere, and two main mechanisms have been proposed to explain coronal heating. The first is wave heating, in which sound, gravitational or magnetohydrodynamic waves are produced by turbulence in the convection zone. These waves travel upward and dissipate in the corona, depositing their energy in the ambient matter in the form of heat. The other is magnetic heating, in which magnetic energy is continuously built up by photospheric motion and released through magnetic reconnection in the form of large solar flares and myriad similar but smaller events—nanoflares.

Currently, it is unclear whether waves are an efficient heating mechanism. All waves except Alfvén waves have been found to dissipate or refract before reaching the corona. In addition, Alfvén waves do not easily dissipate in the corona. Current research focus has therefore shifted towards flare heating mechanisms.

Life phases

Main articles: Formation and evolution of the Solar System and Stellar evolution
See caption
Overview of the evolution of a star like the Sun, from collapsing protostar at left to red giant stage at right

The Sun today is roughly halfway through the main-sequence portion of its life. It has not changed dramatically in over four billion years and will remain fairly stable for about five billion more. However, after hydrogen fusion in its core has stopped, the Sun will undergo dramatic changes, both internally and externally.

Formation

Further information: Formation and evolution of the Solar System

The Sun formed about 4.6 billion years ago from the collapse of part of a giant molecular cloud that consisted mostly of hydrogen and helium and that probably gave birth to many other stars. This age is estimated using computer models of stellar evolution and through nucleocosmochronology. The result is consistent with the radiometric date of the oldest Solar System material, at 4.567 billion years ago. Studies of ancient meteorites reveal traces of stable daughter nuclei of short-lived isotopes, such as iron-60, that form only in exploding, short-lived stars. This indicates that one or more supernovae must have occurred near the location where the Sun formed. A shock wave from a nearby supernova would have triggered the formation of the Sun by compressing the matter within the molecular cloud and causing certain regions to collapse under their own gravity. As one fragment of the cloud collapsed it also began to rotate due to conservation of angular momentum and heat up with the increasing pressure. Much of the mass became concentrated in the center, whereas the rest flattened out into a disk that would become the planets and other Solar System bodies. Gravity and pressure within the core of the cloud generated a lot of heat as it accumulated more matter from the surrounding disk, eventually triggering nuclear fusion.

The stars HD 162826 and HD 186302 share similarities with the Sun and are thus hypothesized to be its stellar siblings, formed in the same molecular cloud.

Main sequence

See caption
Evolution of a Sun-like star. The track of a one solar mass star on the Hertzsprung–Russell diagram is shown from the main sequence to the post-asymptotic-giant-branch stage.

The Sun is about halfway through its main-sequence stage, during which nuclear fusion reactions in its core fuse hydrogen into helium. Each second, more than four billion kilograms of matter are converted into energy within the Sun's core, producing neutrinos and solar radiation. At this rate, the Sun has so far converted around 100 times the mass of Earth into energy, about 0.03% of the total mass of the Sun. The Sun will spend a total of approximately 10 to 11 billion years as a main-sequence star before the red giant phase of the Sun. At the 8 billion year mark, the Sun will be at its hottest point according to the ESA's Gaia space observatory mission in 2022.

The Sun is gradually becoming hotter in its core, hotter at the surface, larger in radius, and more luminous during its time on the main sequence: since the beginning of its main sequence life, it has expanded in radius by 15% and the surface has increased in temperature from 5,620 K (9,660 °F) to 5,772 K (9,930 °F), resulting in a 48% increase in luminosity from 0.677 solar luminosities to its present-day 1.0 solar luminosity. This occurs because the helium atoms in the core have a higher mean molecular weight than the hydrogen atoms that were fused, resulting in less thermal pressure. The core is therefore shrinking, allowing the outer layers of the Sun to move closer to the center, releasing gravitational potential energy. According to the virial theorem, half of this released gravitational energy goes into heating, which leads to a gradual increase in the rate at which fusion occurs and thus an increase in the luminosity. This process speeds up as the core gradually becomes denser. At present, it is increasing in brightness by about 1% every 100 million years. It will take at least 1 billion years from now to deplete liquid water from the Earth from such increase. After that, the Earth will cease to be able to support complex, multicellular life and the last remaining multicellular organisms on the planet will suffer a final, complete mass extinction.

After core hydrogen exhaustion

See caption
The size of the current Sun (now in the main sequence) compared to its estimated size during its red-giant phase in the future

The Sun does not have enough mass to explode as a supernova. Instead, when it runs out of hydrogen in the core in approximately 5 billion years, core hydrogen fusion will stop, and there will be nothing to prevent the core from contracting. The release of gravitational potential energy will cause the luminosity of the Sun to increase, ending the main sequence phase and leading the Sun to expand over the next billion years: first into a subgiant, and then into a red giant. The heating due to gravitational contraction will also lead to expansion of the Sun and hydrogen fusion in a shell just outside the core, where unfused hydrogen remains, contributing to the increased luminosity, which will eventually reach more than 1,000 times its present luminosity. When the Sun enters its red-giant branch (RGB) phase, it will engulf (and very likely destroy) Mercury and Venus. According to a 2008 paper, Earth's orbit will have initially expanded to at most 1.5 AU (220 million km; 140 million mi) due to the Sun's loss of mass. However, Earth's orbit will then start shrinking due to tidal forces (and, eventually, drag from the lower chromosphere) so that it is engulfed by the Sun during the tip of the red-giant branch phase 7.59 billion years from now, 3.8 and 1 million years after Mercury and Venus have respectively suffered the same fate.

By the time the Sun reaches the tip of the red-giant branch, it will be about 256 times larger than it is today, with a radius of 1.19 AU (178 million km; 111 million mi). The Sun will spend around a billion years in the RGB and lose around a third of its mass.

After the red-giant branch, the Sun has approximately 120 million years of active life left, but much happens. First, the core (full of degenerate helium) ignites violently in the helium flash; it is estimated that 6% of the core—itself 40% of the Sun's mass—will be converted into carbon within a matter of minutes through the triple-alpha process. The Sun then shrinks to around 10 times its current size and 50 times the luminosity, with a temperature a little lower than today. It will then have reached the red clump or horizontal branch, but a star of the Sun's metallicity does not evolve blueward along the horizontal branch. Instead, it just becomes moderately larger and more luminous over about 100 million years as it continues to react helium in the core.

When the helium is exhausted, the Sun will repeat the expansion it followed when the hydrogen in the core was exhausted. This time, however, it all happens faster, and the Sun becomes larger and more luminous. This is the asymptotic-giant-branch phase, and the Sun is alternately reacting hydrogen in a shell or helium in a deeper shell. After about 20 million years on the early asymptotic giant branch, the Sun becomes increasingly unstable, with rapid mass loss and thermal pulses that increase the size and luminosity for a few hundred years every 100,000 years or so. The thermal pulses become larger each time, with the later pulses pushing the luminosity to as much as 5,000 times the current level. Despite this, the Sun's maximum AGB radius will not be as large as its tip-RGB maximum: 179 R, or about 0.832 AU (124.5 million km; 77.3 million mi).

Models vary depending on the rate and timing of mass loss. Models that have higher mass loss on the red-giant branch produce smaller, less luminous stars at the tip of the asymptotic giant branch, perhaps only 2,000 times the luminosity and less than 200 times the radius. For the Sun, four thermal pulses are predicted before it completely loses its outer envelope and starts to make a planetary nebula.

The post-asymptotic-giant-branch evolution is even faster. The luminosity stays approximately constant as the temperature increases, with the ejected half of the Sun's mass becoming ionized into a planetary nebula as the exposed core reaches 30,000 K (53,500 °F), as if it is in a sort of blue loop. The final naked core, a white dwarf, will have a temperature of over 100,000 K (180,000 °F) and contain an estimated 54.05% of the Sun's present-day mass. (Simulations indicate that the Sun may be among the least massive stars capable of forming a planetary nebula.) The planetary nebula will disperse in about 10,000 years, but the white dwarf will survive for trillions of years before fading to a hypothetical super-dense black dwarf. As such, it would give off no more energy.

Location

Solar System

Main article: Solar System
Location of the Sun within the Solar System, which extends to the edge of the Oort cloud, where at 125,000 AU to 230,000 AU, equal to several light-years, the Sun's gravitational sphere of influence ends.

The Sun has eight known planets orbiting it. This includes four terrestrial planets (Mercury, Venus, Earth, and Mars), two gas giants (Jupiter and Saturn), and two ice giants (Uranus and Neptune). The Solar System also has nine bodies generally considered as dwarf planets and some more candidates, an asteroid belt, numerous comets, and a large number of icy bodies which lie beyond the orbit of Neptune. Six of the planets and many smaller bodies also have their own natural satellites: in particular, the satellite systems of Jupiter, Saturn, and Uranus are in some ways like miniature versions of the Sun's system.

The Sun is moved by the gravitational pull of the planets. The center of the Sun moves around the Solar System barycenter, within a range from 0.1 to 2.2 solar radii. The Sun's motion around the barycenter approximately repeats every 179 years, rotated by about 30° due primarily to the synodic period of Jupiter and Saturn.

The Sun's gravitational field is estimated to dominate the gravitational forces of surrounding stars out to about two light-years (125,000 AU). Lower estimates for the radius of the Oort cloud, by contrast, do not place it farther than 50,000 AU. Most of the mass is orbiting in the region between 3,000 and 100,000 AU. The furthest known objects, such as Comet West, have aphelia around 70,000 AU from the Sun. The Sun's Hill sphere with respect to the galactic nucleus, the effective range of its gravitational influence, is thought to extend up to a thousand times farther and encompasses the hypothetical Oort cloud. It was calculated by G. A. Chebotarev to be 230,000 AU.

Celestial neighborhood

This section is an excerpt from Solar System § Celestial neighborhood.
Diagram of the Local Interstellar Cloud, the G-Cloud and surrounding stars. As of 2022, the precise location of the Solar System in the clouds is an open question in astronomy.

Within 10 light-years of the Sun there are relatively few stars, the closest being the triple star system Alpha Centauri, which is about 4.4 light-years away and may be in the Local Bubble's G-Cloud. Alpha Centauri A and B are a closely tied pair of Sun-like stars, whereas the closest star to the Sun, the small red dwarf Proxima Centauri, orbits the pair at a distance of 0.2 light-years. In 2016, a potentially habitable exoplanet was found to be orbiting Proxima Centauri, called Proxima Centauri b, the closest confirmed exoplanet to the Sun.

The Solar System is surrounded by the Local Interstellar Cloud, although it is not clear if it is embedded in the Local Interstellar Cloud or if it lies just outside the cloud's edge. Multiple other interstellar clouds exist in the region within 300 light-years of the Sun, known as the Local Bubble. The latter feature is an hourglass-shaped cavity or superbubble in the interstellar medium roughly 300 light-years across. The bubble is suffused with high-temperature plasma, suggesting that it may be the product of several recent supernovae.

The Local Bubble is a small superbubble compared to the neighboring wider Radcliffe Wave and Split linear structures (formerly Gould Belt), each of which are some thousands of light-years in length. All these structures are part of the Orion Arm, which contains most of the stars in the Milky Way that are visible to the unaided eye.

Groups of stars form together in star clusters, before dissolving into co-moving associations. A prominent grouping that is visible to the naked eye is the Ursa Major moving group, which is around 80 light-years away within the Local Bubble. The nearest star cluster is Hyades, which lies at the edge of the Local Bubble. The closest star-forming regions are the Corona Australis Molecular Cloud, the Rho Ophiuchi cloud complex and the Taurus molecular cloud; the latter lies just beyond the Local Bubble and is part of the Radcliffe wave.

Stellar flybys that pass within 0.8 light-years of the Sun occur roughly once every 100,000 years. The closest well-measured approach was Scholz's Star, which approached to ~50,000 AU of the Sun some ~70 thousands years ago, likely passing through the outer Oort cloud. There is a 1% chance every billion years that a star will pass within 100 AU of the Sun, potentially disrupting the Solar System.

Motion

Main article: Galactic year Further information: Stellar kinematics
See caption
The general motion and orientation of the Sun, with Earth and the moon as its Solar System satellites.

The Sun, taking along the whole Solar System, orbits the galaxy's center of mass at an average speed of 230 km/s (828,000 km/h) or 143 mi/s (514,000 mph), taking about 220–250 million Earth years to complete a revolution (a Galactic year), having done so about 20 times since the Sun's formation. The direction of the Sun's motion, the Solar apex, is roughly in the direction of the star Vega.

See caption
The Sun's idealized orbit around the Galactic Center in an artist's top-down depiction of the current layout of the Milky Way.

The Milky Way is moving with respect to the cosmic microwave background radiation (CMB) in the direction of the constellation Hydra with a speed of 550 km/s. Since the sun is moving with respect to the galactic center in the direction of Cygnus (galactic longitude 90°; latitude 0°) at more than 200 km/sec, the resultant velocity with respect to the CMB is about 370 km/s in the direction of Crater or Leo (galactic latitude 264°, latitude 48°).

Observational history

Early understanding

See also: The Sun in culture
A sculpture of the sun in a chariot being pulled by a horse that has wheels instead of hoofs.
The Trundholm sun chariot pulled by a horse is a sculpture believed to be illustrating an important part of Nordic Bronze Age mythology.

In many prehistoric and ancient cultures, the Sun was thought to be a solar deity or other supernatural entity. In the early first millennium BC, Babylonian astronomers observed that the Sun's motion along the ecliptic is not uniform, though they did not know why; it is today known that this is due to the movement of Earth in an elliptic orbit, moving faster when it is nearer to the Sun at perihelion and moving slower when it is farther away at aphelion.

One of the first people to offer a scientific or philosophical explanation for the Sun was the Greek philosopher Anaxagoras. He reasoned that it was a giant flaming ball of metal even larger than the land of the Peloponnesus and that the Moon reflected the light of the Sun. Eratosthenes estimated the distance between Earth and the Sun in the third century BC as "of stadia myriads 400 and 80000", the translation of which is ambiguous, implying either 4,080,000 stadia (755,000 km) or 804,000,000 stadia (148 to 153 million kilometers or 0.99 to 1.02 AU); the latter value is correct to within a few percent. In the first century AD, Ptolemy estimated the distance as 1,210 times the radius of Earth, approximately 7.71 million kilometers (0.0515 AU).

The theory that the Sun is the center around which the planets orbit was first proposed by the ancient Greek Aristarchus of Samos in the third century BC, and later adopted by Seleucus of Seleucia (see Heliocentrism). This view was developed in a more detailed mathematical model of a heliocentric system in the 16th century by Nicolaus Copernicus.

Development of scientific understanding

A drawing of a man wearing a crown in a chariot, being pulled by horses.
Sol, the Sun, from a 1550 edition of Guido Bonatti's Liber astronomiae

Observations of sunspots were recorded during the Han dynasty (206 BC–AD 220) by Chinese astronomers, who maintained records of these observations for centuries. Averroes also provided a description of sunspots in the 12th century. The invention of the telescope in the early 17th century permitted detailed observations of sunspots by Thomas Harriot, Galileo Galilei and other astronomers. Galileo posited that sunspots were on the surface of the Sun rather than small objects passing between Earth and the Sun.

Arabic astronomical contributions include Al-Battani's discovery that the direction of the Sun's apogee (the place in the Sun's orbit against the fixed stars where it seems to be moving slowest) is changing. (In modern heliocentric terms, this is caused by a gradual motion of the aphelion of the Earth's orbit). Ibn Yunus observed more than 10,000 entries for the Sun's position for many years using a large astrolabe.

From an observation of a transit of Venus in 1032, the Persian astronomer and polymath Ibn Sina concluded that Venus was closer to Earth than the Sun. In 1677, Edmond Halley observed a transit of Mercury across the Sun, leading him to realize that observations of the solar parallax of a planet (more ideally using the transit of Venus) could be used to trigonometrically determine the distances between Earth, Venus, and the Sun. Careful observations of the 1769 transit of Venus allowed astronomers to calculate the average Earth–Sun distance as 93,726,900 miles (150,838,800 km), only 0.8% greater than the modern value.

A photograph of the sun
Sun as seen in Hydrogen-alpha light

In 1666, Isaac Newton observed the Sun's light using a prism, and showed that it is made up of light of many colors. In 1800, William Herschel discovered infrared radiation beyond the red part of the solar spectrum. The 19th century saw advancement in spectroscopic studies of the Sun; Joseph von Fraunhofer recorded more than 600 absorption lines in the spectrum, the strongest of which are still often referred to as Fraunhofer lines. The 20th century brought about several specialized systems for observing the Sun, especially at different narrowband wavelengths, such as those using Calcium H (396.9 nm), K (393.37 nm) and Hydrogen-alpha (656.46 nm) filtering.

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 caused by a new element that he dubbed helium, after the Greek Sun god Helios. Twenty-five years later, helium was isolated on Earth.

In the early years of the modern scientific era, the source of the Sun's energy was a significant puzzle. Lord Kelvin suggested that the Sun is a gradually cooling liquid body that is radiating an internal store of heat. Kelvin and Hermann von Helmholtz then proposed a gravitational contraction mechanism to explain the energy output, but the resulting age estimate was only 20 million years, well short of the time span of at least 300 million years suggested by some geological discoveries of that time. In 1890, Lockyer proposed a meteoritic hypothesis for the formation and evolution of the Sun.

Not until 1904 was a documented solution offered. Ernest Rutherford suggested that the Sun's output could be maintained by an internal source of heat, and suggested radioactive decay as the source. However, it would be Albert Einstein who would provide the essential clue to the source of the Sun's energy output with his mass–energy equivalence relation E = mc. In 1920, Sir Arthur Eddington proposed that the pressures and temperatures at the core of the Sun could produce a nuclear fusion reaction that merged hydrogen (protons) into helium nuclei, resulting in a production of energy from the net change in mass. The preponderance of hydrogen in the Sun was confirmed in 1925 by Cecilia Payne using the ionization theory developed by Meghnad Saha. The theoretical concept of fusion was developed in the 1930s by the astrophysicists Subrahmanyan Chandrasekhar and Hans Bethe. Hans Bethe calculated the details of the two main energy-producing nuclear reactions that power the Sun. In 1957, Margaret Burbidge, Geoffrey Burbidge, William Fowler and Fred Hoyle showed that most of the elements in the universe have been synthesized by nuclear reactions inside stars, some like the Sun.

Solar space missions

See also: Solar observatory and List of heliophysics missions
See caption
Illustration of Pioneer 6, 7, 8, and 9

The first satellites designed for long term observation of the Sun from interplanetary space were NASA's Pioneers 6, 7, 8 and 9, which were launched between 1959 and 1968. These probes orbited the Sun at a distance similar to that of Earth, and made the first detailed measurements of the solar wind and the solar magnetic field. Pioneer 9 operated for a particularly long time, transmitting data until May 1983.

In the 1970s, two Helios spacecraft and the Skylab Apollo Telescope Mount provided scientists with significant new data on solar wind and the solar corona. The Helios 1 and 2 probes were U.S.–German collaborations that studied the solar wind from an orbit carrying the spacecraft inside Mercury's orbit at perihelion. The Skylab space station, launched by NASA in 1973, included a solar observatory module called the Apollo Telescope Mount that was operated by astronauts resident on the station. Skylab made the first time-resolved observations of the solar transition region and of ultraviolet emissions from the solar corona. Discoveries included the first observations of coronal mass ejections, then called "coronal transients", and of coronal holes, now known to be intimately associated with the solar wind.

See caption
Drawing of a Solar Maximum Mission probe

In 1980, the Solar Maximum Mission probes were launched by NASA. This spacecraft was designed to observe gamma rays, X-rays and UV radiation from solar flares during a time of high solar activity and solar luminosity. Just a few months after launch, however, an electronics failure caused the probe to go into standby mode, and it spent the next three years in this inactive state. In 1984, Space Shuttle Challenger mission STS-41C retrieved the satellite and repaired its electronics before re-releasing it into orbit. The Solar Maximum Mission subsequently acquired thousands of images of the solar corona before re-entering Earth's atmosphere in June 1989.

Launched in 1991, Japan's Yohkoh (Sunbeam) satellite observed solar flares at X-ray wavelengths. Mission data allowed scientists to identify several different types of flares and demonstrated that the corona away from regions of peak activity was much more dynamic and active than had previously been supposed. Yohkoh observed an entire solar cycle but went into standby mode when an annular eclipse in 2001 caused it to lose its lock on the Sun. It was destroyed by atmospheric re-entry in 2005.

The Solar and Heliospheric Observatory, jointly built by the European Space Agency and NASA, was launched on 2 December 1995. Originally intended to serve a two-year mission, SOHO remains in operation as of 2024. Situated at the Lagrangian point between Earth and the Sun (at which the gravitational pull from both is equal), SOHO has provided a constant view of the Sun at many wavelengths since its launch. Besides its direct solar observation, SOHO has enabled the discovery of a large number of comets, mostly tiny sungrazing comets that incinerate as they pass the Sun.

A photograph of Ulysses spacecraft
Ulysses spacecraft testing at the vacuum spin-balancing facility
See caption
Artist rendition of the Parker Solar Probe

All these satellites have observed the Sun from the plane of the ecliptic, and so have only observed its equatorial regions in detail. The Ulysses probe was launched in 1990 to study the Sun's polar regions. It first traveled to Jupiter, to "slingshot" into an orbit that would take it far above the plane of the ecliptic. Once Ulysses was in its scheduled orbit, it began observing the solar wind and magnetic field strength at high solar latitudes, finding that the solar wind from high latitudes was moving at about 750 km/s, which was slower than expected, and that there were large magnetic waves emerging from high latitudes that scattered galactic cosmic rays.

Elemental abundances in the photosphere are well known from spectroscopic studies, but the composition of the interior of the Sun is more poorly understood. A solar wind sample return mission, Genesis, was designed to allow astronomers to directly measure the composition of solar material.

Observation by eyes

Exposure to the eye

See caption
The Sun seen from Earth, with glare from the lenses. The eye also sees glare when looked towards the Sun directly.

The brightness of the Sun can cause pain from looking at it with the naked eye; however, doing so for brief periods is not hazardous for normal non-dilated eyes. Looking directly at the Sun (sungazing) causes phosphene visual artifacts and temporary partial blindness. It also delivers about 4 milliwatts of sunlight to the retina, slightly heating it and potentially causing damage in eyes that cannot respond properly to the brightness. Viewing of the direct Sun with the naked eye can cause UV-induced, sunburn-like lesions on the retina beginning after about 100 seconds, particularly under conditions where the UV light from the Sun is intense and well focused.

Viewing the Sun through light-concentrating optics such as binoculars may result in permanent damage to the retina without an appropriate filter that blocks UV and substantially dims the sunlight. When using an attenuating filter to view the Sun, the viewer is cautioned to use a filter specifically designed for that use. Some improvised filters that pass UV or IR rays, can actually harm the eye at high brightness levels. Brief glances at the midday Sun through an unfiltered telescope can cause permanent damage.

During sunrise and sunset, sunlight is attenuated because of Rayleigh scattering and Mie scattering from a particularly long passage through Earth's atmosphere, and the Sun is sometimes faint enough to be viewed comfortably with the naked eye or safely with optics (provided there is no risk of bright sunlight suddenly appearing through a break between clouds). Hazy conditions, atmospheric dust, and high humidity contribute to this atmospheric attenuation.

Phenomena

An optical phenomenon, known as a green flash, can sometimes be seen shortly after sunset or before sunrise. The flash is caused by light from the Sun just below the horizon being bent (usually through a temperature inversion) towards the observer. Light of shorter wavelengths (violet, blue, green) is bent more than that of longer wavelengths (yellow, orange, red) but the violet and blue light is scattered more, leaving light that is perceived as green.

Religious aspects

Main article: Solar deity
See caption
Sun and Immortal Birds Gold Ornament by ancient Shu people. The center is a sun pattern with twelve points around which four birds fly in the same counterclockwise direction. Ancient Kingdom of Shu, coinciding with the Shang dynasty.

Solar deities play a major role in many world religions and mythologies. Worship of the Sun was central to civilizations such as the ancient Egyptians, the Inca of South America and the Aztecs of what is now Mexico. In religions such as Hinduism, the Sun is still considered a god, known as Surya. Many ancient monuments were constructed with solar phenomena in mind; for example, stone megaliths accurately mark the summer or winter solstice (for example in Nabta Playa, Egypt; Mnajdra, Malta; and Stonehenge, England); Newgrange, a prehistoric human-built mount in Ireland, was designed to detect the winter solstice; the pyramid of El Castillo at Chichén Itzá in Mexico is designed to cast shadows in the shape of serpents climbing the pyramid at the vernal and autumnal equinoxes.

The ancient Sumerians believed that the Sun was Utu, the god of justice and twin brother of Inanna, the Queen of Heaven, who was identified as the planet Venus. Later, Utu was identified with the East Semitic god Shamash. Utu was regarded as a helper-deity, who aided those in distress.

A painting of Ra and Nefertari
Ra from the tomb of Nefertari, 13th century BC

From at least the Fourth Dynasty of Ancient Egypt, the Sun was worshipped as the god Ra, portrayed as a falcon-headed divinity surmounted by the solar disk, and surrounded by a serpent. In the New Empire period, the Sun became identified with the dung beetle. In the form of the sun disc Aten, the Sun had a brief resurgence during the Amarna Period when it again became the preeminent, if not only, divinity for the Pharaoh Akhenaton. The Egyptians portrayed the god Ra as being carried across the sky in a solar barque, accompanied by lesser gods, and to the Greeks, he was Helios, carried by a chariot drawn by fiery horses. From the reign of Elagabalus in the late Roman Empire the Sun's birthday was a holiday celebrated as Sol Invictus (literally "Unconquered Sun") soon after the winter solstice, which may have been an antecedent to Christmas. Regarding the fixed stars, the Sun appears from Earth to revolve once a year along the ecliptic through the zodiac, and so Greek astronomers categorized it as one of the seven planets (Greek planetes, "wanderer"); the naming of the days of the weeks after the seven planets dates to the Roman era.

In Proto-Indo-European religion, the Sun was personified as the goddess *Seh2ul. Derivatives of this goddess in Indo-European languages include the Old Norse Sól, Sanskrit Surya, Gaulish Sulis, Lithuanian Saulė, and Slavic Solntse. In ancient Greek religion, the sun deity was the male god Helios, who in later times was syncretized with Apollo.

In the Bible, Malachi 4:2 mentions the "Sun of Righteousness" (sometimes translated as the "Sun of Justice"), which some Christians have interpreted as a reference to the Messiah (Christ). In ancient Roman culture, Sunday was the day of the sun god. In paganism, the Sun was a source of life, giving warmth and illumination. It was the center of a popular cult among Romans, who would stand at dawn to catch the first rays of sunshine as they prayed. The celebration of the winter solstice (which influenced Christmas) was part of the Roman cult of the unconquered Sun (Sol Invictus). It was adopted as the Sabbath day by Christians. The symbol of light was a pagan device adopted by Christians, and perhaps the most important one that did not come from Jewish traditions. Christian churches were built so that the congregation faced toward the sunrise.

Tonatiuh, the Aztec god of the sun, was closely associated with the practice of human sacrifice. The sun goddess Amaterasu is the most important deity in the Shinto religion, and she is believed to be the direct ancestor of all Japanese emperors.

See also

Notes

  1. ^ All numbers in this article are short scale. One billion is 10, or 1,000,000,000.
  2. In astronomical sciences, the term heavy elements (or metals) refers to all chemical elements except hydrogen and helium.
  3. Hydrothermal vent communities live so deep under the sea that they have no access to sunlight. Bacteria instead use sulfur compounds as an energy source, via chemosynthesis.
  4. Counterclockwise is also the direction of revolution around the Sun for objects in the Solar System and is the direction of axial spin for most objects.
  5. Earth's atmosphere near sea level has a particle density of about 2×10 m.

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