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{{short description|Unit of length used in astronomy and is defined as : The distance at which 1 AU subtends an angle of 1 arc second}}
{{short description|Unit of length used in astronomy}}
{{Other uses}}
{{Other uses}}
{{Use dmy dates|date=May 2020}}
{{Use dmy dates|date=May 2020}}
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| symbol = pc
| symbol = pc
| units1 = [[metric system|metric]] ([[International System of Units|SI]]) units
| units1 = [[metric system|metric]] ([[International System of Units|SI]]) units
| inunits1 = {{Val|3.0857|e=16|ul=m}} <br />&nbsp;&nbsp;&nbsp;~31 [[petametres]]
| inunits1 = {{convert|1|pc|m|disp=out|sigfig=5|lk=on}} <br />{{nbsp|3}}≈{{convert|1|pc|Pm|disp=out|sigfig=2|abbr=off|lk=on}}
| units2 = [[Imperial units|imperial]]&nbsp;&&nbsp;[[United States customary units|US]]&nbsp;units
| units2 = [[Imperial units|imperial]]&nbsp;&nbsp;[[United States customary units|US]]&nbsp;units
| inunits2 = {{Val|1.9174|e=13|ul=mi}}
| inunits2 = {{convert|1|pc|mi|disp=out|sigfig=5|lk=on}}
| units3 = [[Astronomical system of units|astronomical units]]
| units3 = [[Astronomical system of units|astronomical units]]
| inunits3 = {{Val|2.06265|e=5|ul=au}}<br />&nbsp;&nbsp;&nbsp;{{Val|3.26156|ul=ly}}
| inunits3 = {{convert|1|pc|au|disp=out|sigfig=6|lk=on}}<br />{{nbsp|3}}{{convert|1|pc|ly|disp=out|sigfig=6|lk=on}}
}}
}}


The '''parsec''' (symbol: '''pc''') is a [[unit of length]] used to measure the large distances to [[astronomical object]]s outside the [[Solar System]], approximately equal to {{convert|1|pc|ly|2|abbr=off|lk=out|disp=out}} or {{convert|1|pc|AU|0|abbr=off|lk=out|disp=out}} (au), i.e. {{convert|30.9|e12km|e12mi|abbr=off|lk=on}}.{{efn|name=trillion|One trillion here is [[long and short scales|short scale]], ie. 10<sup>12</sup> (one million million, or billion in long scale).}} The parsec unit is obtained by the use of [[parallax]] and [[trigonometry]], and is defined as the distance at which 1 au [[subtended angle|subtends]] an angle of one [[arcsecond]]<ref>{{Cite web |title=Cosmic Distance Scales – The Milky Way |url=https://heasarc.gsfc.nasa.gov/docs/cosmic/milkyway_info.html |access-date=24 September 2014}}</ref> ({{sfrac|3600}} of a [[degree (angle)|degree]]). This corresponds to {{sfrac|{{Val|648000}}|{{pi}}}} astronomical units, i.e. <math>1\, \mathrm{pc} = 1~\mathrm{au}/\tan \left({1} \ \mathrm{arcsec} \right)</math>.<ref name="au_parsec">{{Cite journal |last1=B. Luque |last2=F. J. Ballesteros |date=2019 |title= To the Sun and beyond |journal=[[Nature Physics]] |volume=15 |issue=12 |pages=1302 |doi=10.1038/s41567-019-0685-3 |bibcode=2019NatPh..15.1302L |doi-access=free}}</ref> The nearest star, [[Proxima Centauri]], is about {{convert|1.3|pc|ly|abbr=off}} from the [[Sun]].<ref>{{Cite conference |last=Benedict |first=G.&nbsp;F. |display-authors=etal |title=Astrometric Stability and Precision of Fine Guidance Sensor #3: The Parallax and Proper Motion of Proxima Centauri | url = http://clyde.as.utexas.edu/SpAstNEW/Papers_in_pdf/%7BBen93%7DEarlyProx.pdf |pages=380–384 |access-date=11 July 2007 |book-title=Proceedings of the HST Calibration Workshop}}</ref> Most [[Naked-eye stars|stars visible to the naked eye]] are within a few hundred parsecs of the Sun, with the most distant at a few thousand.<ref>{{cite web |title=Farthest Stars |url=https://stardate.org/radio/program/2021-05-15 |website=[[StarDate]] |publisher=[[University of Texas at Austin]] |access-date=5 September 2021 |date=15 May 2021}}</ref>
The '''parsec''' (symbol: '''pc''') is a [[unit of length]] used to measure the large distances to [[astronomical object]]s outside the [[Solar System]], approximately equal to {{convert|1|pc|ly|2|abbr=off|lk=out|disp=out}} or {{convert|1|pc|AU|0|abbr=off|lk=out|disp=out}} (AU), i.e. {{convert|30.9|e12km|e12mi|abbr=off|lk=on}}.{{efn|name=trillion|One trillion here is [[long and short scales|short scale]], ie. 10<sup>12</sup> (one million million, or billion in long scale).}} The parsec unit is obtained by the use of [[parallax]] and [[trigonometry]], and is defined as the distance at which 1 AU [[subtended angle|subtends]] an angle of one [[arcsecond]]<ref>{{Cite web |title=Cosmic Distance Scales – The Milky Way |url=https://heasarc.gsfc.nasa.gov/docs/cosmic/milkyway_info.html |access-date=24 September 2014}}</ref> ({{sfrac|3600}} of a [[degree (angle)|degree]]). The nearest star, [[Proxima Centauri]], is about {{convert|1.3|pc|ly|abbr=off}} from the [[Sun]]: from that distance, the gap between the Earth and the Sun spans slightly less than {{sfrac|3600}} of one degree of view.<ref>{{Cite conference |last=Benedict |first=G.&nbsp;F. |display-authors=etal |title=Astrometric Stability and Precision of Fine Guidance Sensor #3: The Parallax and Proper Motion of Proxima Centauri | url = http://clyde.as.utexas.edu/SpAstNEW/Papers_in_pdf/%7BBen93%7DEarlyProx.pdf |pages=380–384 |access-date=11 July 2007 |book-title=Proceedings of the HST Calibration Workshop}}</ref> Most [[Naked-eye stars|stars visible to the naked eye]] are within a few hundred parsecs of the Sun, with the most distant at a few thousand parsecs, and the [[Andromeda Galaxy]] at over 700,000 parsecs.<ref>{{cite web |title=Farthest Stars |url=https://stardate.org/radio/program/2021-05-15 |website=[[StarDate]] |publisher=[[University of Texas at Austin]] |access-date=5 September 2021 |date=15 May 2021}}</ref>


The word ''parsec'' is a [[portmanteau]] of "parallax of one second" and was coined by the British astronomer [[Herbert Hall Turner]] in 1913<ref name="dyson">{{Cite journal |last=Dyson |first=F.&nbsp;W. |author-link=Frank Watson Dyson |date=March 1913 |title= The distribution in space of the stars in Carrington's Circumpolar Catalogue |journal= [[Monthly Notices of the Royal Astronomical Society]] |volume=73 |issue=5 |page=342 <!-- the whole article is at pp.=334–345 but single page in the source that supports the content" has preference. Note that both OUP.com and Harvard.edu PDFs are truncated at p. 342 --> | bibcode=1913MNRAS..73..334D |doi=10.1093/mnras/73.5.334 |doi-access=free | quote= [''paragraph 14, page 342''] Taking the unit of distance R* to be that corresponding to a parallax of 1″·0 [… Footnote:] <br> * There is need for a name for this unit of distance. Mr. [[Carl Charlier|Charlier]] has suggested [[Sirius|Sirio]]meter, but if the violence to the Greek language can be overlooked, the word ''Astron'' might be adopted. Professor [[Herbert Hall Turner|Turner]] suggests ''Parsec'', which may be taken as an abbreviated form of "a distance corresponding to a parallax of one second".}}</ref> to make calculations of astronomical distances from only raw observational data easy for astronomers. Partly for this reason, it is the unit preferred in [[astronomy]] and [[astrophysics]], though the [[light-year]] remains prominent in [[popular science]] texts and common [[usage]]. Although parsecs are used for the shorter distances within the [[Milky Way]], multiples of parsecs are required for the larger scales in the universe, including [[kilo-|kilo]]<nowiki/>parsecs (kpc) for the more distant objects within and around the Milky Way, [[Mega-|mega]]<nowiki/>parsecs (Mpc) for mid-distance galaxies, and [[giga-|giga]]<nowiki/>parsecs (Gpc) for many [[quasar]]s and the most distant galaxies.
The word ''parsec'' is a [[portmanteau]] of "parallax of one second" and was coined by the British astronomer [[Herbert Hall Turner]] in 1913<ref name="dyson">{{Cite journal |last=Dyson |first=F.&nbsp;W. |author-link=Frank Watson Dyson |date=March 1913 |title= The distribution in space of the stars in Carrington's Circumpolar Catalogue |journal= [[Monthly Notices of the Royal Astronomical Society]] |volume=73 |issue=5 |page=342 <!-- the whole article is at pp.=334–345 but single page in the source that supports the content" has preference. Note that both OUP.com and Harvard.edu PDFs are truncated at p. 342 --> | bibcode=1913MNRAS..73..334D |doi=10.1093/mnras/73.5.334 |doi-access=free | quote= [''paragraph 14, page 342''] Taking the unit of distance R* to be that corresponding to a parallax of 1″·0 [… Footnote:] <br> * There is need for a name for this unit of distance. Mr. [[Carl Charlier|Charlier]] has suggested [[Sirius|Sirio]]meter, but if the violence to the Greek language can be overlooked, the word ''Astron'' might be adopted. Professor [[Herbert Hall Turner|Turner]] suggests ''Parsec'', which may be taken as an abbreviated form of "a distance corresponding to a parallax of one second".}}</ref> to simplify astronomers' calculations of astronomical distances from only raw observational data. Partly for this reason, it is the unit preferred in [[astronomy]] and [[astrophysics]], though the [[light-year]] remains prominent in [[popular science]] texts and common usage. Although parsecs are used for the shorter distances within the [[Milky Way]], multiples of parsecs are required for the larger scales in the universe, including [[kilo-|kilo]]<nowiki/>parsecs (kpc) for the more distant objects within and around the Milky Way, [[Mega-|mega]]<nowiki/>parsecs (Mpc) for mid-distance galaxies, and [[giga-|giga]]<nowiki/>parsecs (Gpc) for many [[quasar]]s and the most distant galaxies.


In August 2015, the [[International Astronomical Union]] (IAU) passed Resolution B2 which, as part of the definition of a standardized absolute and apparent [[bolometric magnitude]] scale, mentioned an existing explicit definition of the parsec as exactly {{sfrac|{{Val|648000}}|{{pi}}}}&nbsp;au, or approximately {{Val|30.856775814913673|e=15}}<!-- if absurdly many digits are needed, let the full listing correspond to rounded meters -->&nbsp;metres (based on the IAU 2012 exact SI definition of the astronomical unit). This corresponds to the small-angle definition of the parsec found in many astronomical references.<ref>{{Cite book |title=Allen's Astrophysical Quantities |date=2000 |publisher=AIP Press / Springer |isbn=978-0387987460 |editor-last=Cox |editor-first=Arthur N. |edition=4th |location=New York |bibcode=2000asqu.book.....C}}</ref><ref>{{Cite book |last1=Binney |first1=James |title=Galactic Dynamics |last2=Tremaine |first2=Scott |date=2008 |publisher=Princeton University Press |isbn=978-0-691-13026-2 |edition=2nd |location=Princeton, NJ |bibcode=2008gady.book.....B}}</ref>
In August 2015, the [[International Astronomical Union]] (IAU) passed Resolution B2 which, as part of the definition of a standardized absolute and apparent [[bolometric magnitude]] scale, mentioned an existing explicit definition of the parsec as exactly {{sfrac|{{Val|648000}}|{{pi}}}}&nbsp;au, or approximately {{Val|3.0856775814913673|e=16}}<!-- if absurdly many digits are needed, let the full listing correspond to rounded meters -->&nbsp;metres (based on the IAU 2012 definition of the astronomical unit). This corresponds to the small-angle definition of the parsec found in many astronomical references.<ref>{{Cite book |title=Allen's Astrophysical Quantities |date=2000 |publisher=AIP Press / Springer |isbn=978-0387987460 |editor-last=Cox |editor-first=Arthur N. |edition=4th |location=New York |bibcode=2000asqu.book.....C}}</ref><ref>{{Cite book |last1=Binney |first1=James |title=Galactic Dynamics |last2=Tremaine |first2=Scott |date=2008 |publisher=Princeton University Press |isbn=978-0-691-13026-2 |edition=2nd |location=Princeton, NJ |bibcode=2008gady.book.....B}}</ref>


== History and derivation ==
== History and derivation ==
{{See also|Stellar parallax}}
{{See also|Stellar parallax}}
Imagining an elongated [[right triangle]] in space, where the shorter leg measures one au ([[astronomical unit]], the average [[Earth]]–[[Sun]] distance) and the [[subtended|subtended angle]] of the vertex opposite that leg measures one [[arcsecond]] ({{frac|3600}} of a degree), the parsec is defined as the length of the [[Trigonometry#Trigonometric_ratios|''adjacent'']] leg. The value of a parsec can be derived through the rules of [[trigonometry]]. The distance from Earth whereupon the radius of its solar orbit subtends one arcsecond.
{{Repetition section|date=May 2020}}


One of the oldest methods used by astronomers to calculate the distance to a [[star]] is to record the difference in angle between two measurements of the position of the star in the sky. The first measurement is taken from the Earth on one side of the Sun, and the second is taken approximately half a year later, when the Earth is on the opposite side of the Sun.{{efn|name=orbit|Terrestrial observations of a star's position should be taken when the Earth is at the furthest points in its orbit from a line between the Sun and the star, in order to form a right angle at the Sun and a full au of separation as viewed from the star.}} The distance between the two positions of the Earth when the two measurements were taken is twice the distance between the Earth and the Sun. The difference in angle between the two measurements is twice the parallax angle, which is formed by lines from the Sun and Earth to the star at the distant [[Vertex (geometry)#Of an angle|vertex]]. Then the distance to the star could be calculated using trigonometry.<ref name="NASAparallax">{{Cite web |title=Deriving the Parallax Formula |url=http://imagine.gsfc.nasa.gov/YBA/HTCas-size/parallax1-derive.html |last=[[High Energy Astrophysics Science Archive Research Center]] (HEASARC) |website=NASA's Imagine the Universe! |publisher=Astrophysics Science Division (ASD) at [[NASA]]'s [[Goddard Space Flight Center]] |access-date=26 November 2011}}</ref> The first successful published direct measurements of an object at interstellar distances were undertaken by German astronomer [[Friedrich Wilhelm Bessel]] in 1838, who used this approach to calculate the 3.5-parsec distance of [[61&nbsp;Cygni]].<ref>{{Cite journal |last=Bessel |first=F.&nbsp;W. |author-link=Friedrich Wilhelm Bessel |date=1838 |title=Bestimmung der Entfernung des 61sten Sterns des Schwans |trans-title=Determination of the distance of the 61st star of Cygnus |url=https://zenodo.org/record/1424605 |url-status= |journal=[[Astronomische Nachrichten]] |volume=16 |issue=5 |pages=65–96 |bibcode=1838AN.....16...65B |doi=10.1002/asna.18390160502 |archive-url= |archive-date=}}</ref>
The parsec is defined as being equal to the length of the adjacent leg (opposite leg being 1 AU) of an extremely elongated imaginary [[right triangle]] in space. The two dimensions on which this triangle is based are its shorter leg, of length one [[astronomical unit]] (the average [[Earth]]-[[Sun]] distance), and the [[subtended|subtended angle]] of the vertex opposite that leg, measuring one [[arcsecond]]. Applying the rules of [[trigonometry]] to these two values, the unit length of the other leg of the triangle (the parsec) can be derived.


[[Image:ParallaxV2.svg|thumb|left|upright=1.36|Stellar parallax motion from annual parallax|alt=Diagrams illustrating the apparent change in position of a celestial object when viewed from different positions in Earth's orbit.]]
One of the oldest methods used by astronomers to calculate the distance to a [[star]] is to record the difference in angle between two measurements of the position of the star in the sky. The first measurement is taken from the Earth on one side of the Sun, and the second is taken approximately half a year later, when the Earth is on the opposite side of the Sun. The distance between the two positions of the Earth when the two measurements were taken is twice the distance between the Earth and the Sun. The difference in angle between the two measurements is twice the parallax angle, which is formed by lines from the Sun and Earth to the star at the distant [[Vertex (geometry)#Of an angle|vertex]]. Then the distance to the star could be calculated using trigonometry.<ref name="NASAparallax">{{Cite web |title=Deriving the Parallax Formula |url=http://imagine.gsfc.nasa.gov/YBA/HTCas-size/parallax1-derive.html |last=[[High Energy Astrophysics Science Archive Research Center]] (HEASARC) |website=NASA's Imagine the Universe! |publisher=Astrophysics Science Division (ASD) at [[NASA]]'s [[Goddard Space Flight Center]] |access-date=26 November 2011}}</ref> The first successful published direct measurements of an object at interstellar distances were undertaken by German astronomer [[Friedrich Wilhelm Bessel]] in 1838, who used this approach to calculate the 3.5-parsec distance of [[61 Cygni]].<ref>{{Cite journal |last=Bessel |first=F.&nbsp;W. |author-link=Friedrich Wilhelm Bessel |date=1838 |title=Bestimmung der Entfernung des 61sten Sterns des Schwans |trans-title=Determination of the distance of the 61st star of Cygnus |url=http://www.ari.uni-heidelberg.de/gaia/documents/bessel-1838/index.html |url-status=dead |journal=[[Astronomische Nachrichten]] |volume=16 |issue=5 |pages=65–96 |bibcode=1838AN.....16...65B |doi=10.1002/asna.18390160502 |archive-url=https://web.archive.org/web/20070624220502/http://www.ari.uni-heidelberg.de/gaia/documents/bessel-1838/index.html |archive-date=24 June 2007}}</ref>
The parallax of a star is defined as half of the [[angular distance]] that a star appears to move relative to the [[celestial sphere]] as Earth orbits the Sun. Equivalently, it is the subtended angle, from that star's perspective, of the [[semimajor axis]] of the Earth's orbit. Substituting the star's parallax for the one arcsecond angle in the imaginary right triangle, the long leg of the triangle will measure the distance from the Sun to the star. A parsec can be defined as the length of the right triangle side adjacent to the vertex occupied by a star whose parallax angle is one arcsecond.


The use of the parsec as a unit of distance follows naturally from Bessel's method, because the distance in parsecs can be computed simply as the [[multiplicative inverse|reciprocal]] of the parallax angle in arcseconds (i.e.: if the parallax angle is 1&nbsp;arcsecond, the object is 1&nbsp;pc from the Sun; if the parallax angle is 0.5&nbsp;arcseconds, the object is 2&nbsp;pc away; etc.). No [[trigonometric function]]s are required in this relationship because the very small angles involved mean that the approximate solution of the [[skinny triangle]] can be applied.
[[Image:ParallaxV2.svg|thumb|left|upright=1.36|Stellar parallax motion from annual parallax]]
The parallax of a star is defined as half of the [[angular distance]] that a star appears to move relative to the [[celestial sphere]] as Earth orbits the Sun. Equivalently, it is the subtended angle, from that star's perspective, of the [[semimajor axis]] of the Earth's orbit. The star, the Sun and the Earth form the corners of an imaginary right triangle in space: the right angle is the corner at the Sun, and the corner at the star is the parallax angle. The length of the opposite side to the parallax angle is the distance from the Earth to the Sun (defined as one astronomical unit, au), and the length of the [[Adjacent side (right triangle)#Trigonometric ratios in right triangles|adjacent]] side gives the distance from the sun to the star. Therefore, given a measurement of the parallax angle, along with the rules of trigonometry, the distance from the Sun to the star can be found. A parsec is defined as the length of the side adjacent to the vertex occupied by a star whose parallax angle is one arcsecond.

The use of the parsec as a unit of distance follows naturally from Bessel's method, because the distance in parsecs can be computed simply as the [[multiplicative inverse|reciprocal]] of the parallax angle in arcseconds (i.e. if the parallax angle is 1&nbsp;arcsecond, the object is 1&nbsp;pc from the Sun; if the parallax angle is 0.5&nbsp;arcseconds, the object is 2&nbsp;pc away; etc.). No [[trigonometric function]]s are required in this relationship because the very small angles involved mean that the approximate solution of the [[skinny triangle]] can be applied.


Though it may have been used before, the term ''parsec'' was first mentioned in an astronomical publication in 1913. [[Astronomer Royal]] [[Frank Watson Dyson]] expressed his concern for the need of a name for that unit of distance. He proposed the name ''astron'', but mentioned that [[Carl Charlier]] had suggested ''[[siriometer]]'' and [[Herbert Hall Turner]] had proposed ''parsec''.<ref name=dyson /> It was Turner's proposal that stuck.
Though it may have been used before, the term ''parsec'' was first mentioned in an astronomical publication in 1913. [[Astronomer Royal]] [[Frank Watson Dyson]] expressed his concern for the need of a name for that unit of distance. He proposed the name ''astron'', but mentioned that [[Carl Charlier]] had suggested ''[[siriometer]]'' and [[Herbert Hall Turner]] had proposed ''parsec''.<ref name=dyson /> It was Turner's proposal that stuck.
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Therefore,
Therefore,
<math display="block">\pi ~ \mathrm{pc} = 180 \times 60 \times 60 ~ \mathrm{au} = 180 \times 60 \times 60 \times 149\,597\,870\,700 ~ \mathrm{m} = 96\,939\,420\,213\,600\,000 ~ \mathrm{m}</math> (exact by the 2015 definition)

:<math>\pi ~ \mathrm{pc} = 180 \times 60 \times 60 ~ \mathrm{au} = 180 \times 60 \times 60 \times 149\,597\,870\,700 ~ \mathrm{m} = 96\,939\,420\,213\,600\,000 ~ \mathrm{m}</math> (exact by the 2015 definition)


Therefore,
Therefore,


<math display=block>1 ~ \mathrm{pc} = \frac{96\,939\,420\,213\,600\,000}{\pi} ~ \mathrm{m} = 30\,856\,775\,814\,913\,673 ~ \mathrm{m}</math> (to the nearest [[metre]])
<math display=block>1 ~ \mathrm{pc} = \frac{96\,939\,420\,213\,600\,000}{\pi} ~ \mathrm{m} = 30\,856\,775\,814\,913\,673 ~ \mathrm{m}</math> (to the nearest [[metre]]).


Approximately,
Approximately,
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:[[Image:Parsec (1).svg|400px|Diagram of parsec.]]
:[[Image:Parsec (1).svg|400px|Diagram of parsec.]]


In the diagram above (not to scale), '''S''' represents the Sun, and '''E''' the Earth at one point in its orbit. Thus the distance '''ES''' is one astronomical unit (au). The angle '''SDE''' is one arcsecond ({{sfrac|3600}} of a [[degree (angle)|degree]]) so by definition '''D''' is a point in space at a distance of one parsec from the Sun. Through trigonometry, the distance '''SD''' is calculated as follows:
In the diagram above (not to scale), '''S''' represents the Sun, and '''E''' the Earth at one point in its orbit (such as to form a right angle at '''S'''{{efn|name=orbit}}). Thus the distance '''ES''' is one astronomical unit (au). The angle '''SDE''' is one arcsecond ({{sfrac|3600}} of a [[degree (angle)|degree]]) so by definition '''D''' is a point in space at a distance of one parsec from the Sun. Through trigonometry, the distance '''SD''' is calculated as follows:


<math display=block>
<math display=block>
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: Then {{Val|1|u=pc}} ≈ {{Val|3.261563777|u=ly}}
: Then {{Val|1|u=pc}} ≈ {{Val|3.261563777|u=ly}}


A corollary states that a parsec is also the distance from which a disc one astronomical unit in diameter must be viewed for it to have an [[angular diameter]] of one arcsecond (by placing the observer at '''D''' and a diameter of the disc on '''ES''').
A corollary states that a parsec is also the distance from which a disc that is one au in diameter must be viewed for it to have an [[angular diameter]] of one arcsecond (by placing the observer at '''D''' and a disc spanning '''ES''').


Mathematically, to calculate distance, given obtained angular measurements from instruments in arcseconds, the formula would be:
Mathematically, to calculate distance, given obtained angular measurements from instruments in arcseconds, the formula would be:
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where ''θ'' is the measured angle in arcseconds, Distance<sub>earth-sun</sub> is a constant ({{Val|1|u=au}} or {{Convert|1|au|ly|disp=out|sigfig=5}}). The calculated stellar distance will be in the same measurement unit as used in Distance<sub>earth-sun</sub> (e.g. if Distance<sub>earth-sun</sub> = {{Val|1|u=au}}, unit for Distance<sub>star</sub> is in astronomical units; if Distance<sub>earth-sun</sub> = {{Convert|1|au|ly|disp=out|sigfig=5}}, unit for Distance<sub>star</sub> is in light-years).
where ''θ'' is the measured angle in arcseconds, Distance<sub>earth-sun</sub> is a constant ({{Val|1|u=au}} or {{Convert|1|au|ly|disp=out|sigfig=5}}). The calculated stellar distance will be in the same measurement unit as used in Distance<sub>earth-sun</sub> (e.g. if Distance<sub>earth-sun</sub> = {{Val|1|u=au}}, unit for Distance<sub>star</sub> is in astronomical units; if Distance<sub>earth-sun</sub> = {{Convert|1|au|ly|disp=out|sigfig=5}}, unit for Distance<sub>star</sub> is in light-years).


The length of the parsec used in [[IAU]] 2015 Resolution B2<ref>{{Citation |title=RESOLUTION B2 |date=13 August 2015 |editor-last=International Astronomical Union |contribution=RESOLUTION B2 on recommended zero points for the absolute and apparent bolometric magnitude scales |contribution-url=http://www.iau.org/enwiki/static/resolutions/IAU2015_English.pdf |place=Honolulu |publisher=[[International Astronomical Union]] |quote=The XXIX General Assembly of the International Astronomical Union notes [4] that the parsec is defined as exactly (648 000/<math>\pi</math>) au per the AU definition in IAU 2012 Resolution B2}}</ref> (exactly {{sfrac|{{Val|648000}}|{{pi}}}} astronomical units) corresponds exactly to that derived using the small-angle calculation. This differs from the classic inverse-[[tangent]] definition by about {{Val|200|u=km}}, i.e. only after the 11th [[significant figure]]. As the astronomical unit was defined by the IAU (2012) as an exact [[SI]] length in metres, so now the parsec corresponds to an exact SI length in metres. To the nearest meter, the small-angle parsec corresponds to {{Val|30856775814913673|u=m}}.
The length of the parsec used in [[IAU]] 2015 Resolution B2<ref>{{Citation |title=RESOLUTION B2 |date=13 August 2015 |editor-last=International Astronomical Union |contribution=RESOLUTION B2 on recommended zero points for the absolute and apparent bolometric magnitude scales |contribution-url=http://www.iau.org/enwiki/static/resolutions/IAU2015_English.pdf |place=Honolulu |publisher=[[International Astronomical Union]] |quote=The XXIX General Assembly of the International Astronomical Union notes [4] that the parsec is defined as exactly (648 000/<math>\pi</math>) au per the AU definition in IAU 2012 Resolution B2}}</ref> (exactly {{sfrac|{{Val|648000}}|{{pi}}}} astronomical units) corresponds exactly to that derived using the small-angle calculation. This differs from the classic inverse-[[tangent]] definition by about {{Val|200|u=km}}, i.e.: only after the 11th [[significant figure]]. As the astronomical unit was defined by the IAU (2012) as an exact length in metres, so now the parsec corresponds to an exact length in metres. To the nearest meter, the small-angle parsec corresponds to {{Val|30856775814913673|u=m}}.


== Usage and measurement ==
== Usage and measurement ==
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<!-- [[NASA]]'s [[Full-sky Astrometric Mapping Explorer|''FAME'' satellite]] was to have been launched in 2004, to measure parallaxes for about 40&nbsp;million stars with sufficient precision to measure stellar distances of up to 2000&nbsp;pc. However, the mission's funding was withdrawn by NASA in January 2002.<ref>[http://www.usno.navy.mil/FAME/news/ FAME news], 25 January 2002.</ref> -->
<!-- [[NASA]]'s [[Full-sky Astrometric Mapping Explorer|''FAME'' satellite]] was to have been launched in 2004, to measure parallaxes for about 40&nbsp;million stars with sufficient precision to measure stellar distances of up to 2000&nbsp;pc. However, the mission's funding was withdrawn by NASA in January 2002.<ref>[http://www.usno.navy.mil/FAME/news/ FAME news], 25 January 2002.</ref> -->
ESA's [[Gaia mission|''Gaia'' satellite]], which launched on 19 December 2013, is intended to measure one billion stellar distances to within {{Val|20|u=microarcsecond}}, producing errors of 10% in measurements as far as the [[Galactic Center|Galactic Centre]], about {{Val|8000|u=pc}} away in the [[constellation]] of [[Sagittarius (constellation)|Sagittarius]].<ref>{{Cite web |title=GAIA |url=http://sci.esa.int/science-e/www/area/index.cfm?fareaid=26 |publisher=[[European Space Agency]]}}</ref>
ESA's [[Gaia mission|''Gaia'' satellite]], which launched on 19 December 2013, is intended to measure one billion stellar distances to within {{Val|20|u=microarcsecond}}s, producing errors of 10% in measurements as far as the [[Galactic Center|Galactic Centre]], about {{Val|8000|u=pc}} away in the [[constellation]] of [[Sagittarius (constellation)|Sagittarius]].<ref>{{Cite web |title=GAIA |url=http://sci.esa.int/science-e/www/area/index.cfm?fareaid=26 |publisher=[[European Space Agency]]}}</ref>


== Distances in parsecs ==
== Distances in parsecs ==
Line 105: Line 102:
Distances expressed in fractions of a parsec usually involve objects within a single star system. So, for example:
Distances expressed in fractions of a parsec usually involve objects within a single star system. So, for example:
* One astronomical unit (au), the distance from the Sun to the Earth, is just under {{Val|5|e=-6|u=parsec}}.
* One astronomical unit (au), the distance from the Sun to the Earth, is just under {{Val|5|e=-6|u=parsec}}.
* The most distant [[space probe]], ''[[Voyager 1]]'', was {{Val|0.000703|u=parsec}} from Earth {{As of|January 2019|lc=on}}. ''Voyager 1'' took {{Val|41|u=years}} to cover that distance.
* The most distant [[space probe]], ''[[Voyager 1]]'', was {{Val|0.0007897|u=parsec}} from Earth {{As of|2024|February|lc=on}}. ''Voyager 1'' took {{Val|46|u=years}} to cover that distance.
* The [[Oort cloud]] is estimated to be approximately {{Val|0.6|u=parsec}} in [[diameter]]
* The [[Oort cloud]] is estimated to be approximately {{Val|0.6|u=parsec}} in [[diameter]]


Line 111: Line 108:


=== Parsecs and kiloparsecs ===
=== Parsecs and kiloparsecs ===
{{Unreferenced section|date=June 2024}}
Distances expressed in parsecs (pc) include distances between nearby stars, such as those in the same [[spiral arm]] or [[globular cluster]]. A distance of {{Convert|1000|pc|ly|sigfig=4}} is denoted by the kiloparsec (kpc). Astronomers typically use kiloparsecs to express distances between parts of a [[galaxy]], or within [[galaxy group|groups of galaxies]]. So, for example (NB one parsec is approximately equal to {{Convert|1|pc|ly|sigfig=3|disp=out|abbr=off}}):
Distances expressed in parsecs (pc) include distances between nearby stars, such as those in the same [[spiral arm]] or [[globular cluster]]. A distance of {{Convert|1000|pc|ly|sigfig=4}} is denoted by the kiloparsec (kpc). Astronomers typically use kiloparsecs to express distances between parts of a [[galaxy]] or within [[galaxy group|groups of galaxies]]. So, for example :
* [[Proxima Centauri]], the nearest known star to earth other than the sun, is about {{Convert|1.3|pc|ly|sigfig=3}} away, by direct parallax measurement.
* The distance to the [[open cluster]] [[Pleiades]] is {{Val|130|10|u=pc}} ({{Val|420|30|u=ly}}) from us, per ''[[Hipparcos]]'' parallax measurement.
* [[Proxima Centauri]], the nearest known star to Earth other than the Sun, is about {{Convert|1.3|pc|ly|sigfig=3}} away by direct parallax measurement.
* The distance to the [[open cluster]] [[Pleiades]] is {{Val|130|10|u=pc}} ({{Val|420|30|u=ly}}) from us per ''[[Hipparcos]]'' parallax measurement.
* The [[Galactic Center|centre]] of the [[Milky Way]] is more than {{Convert|8|kpc|ly}} from the Earth, and the Milky Way is roughly {{Convert|34|kpc|ly}} across.
* The [[Galactic Center|centre]] of the [[Milky Way]] is more than {{Convert|8|kpc|ly}} from the Earth and the Milky Way is roughly {{Convert|34|kpc|ly}} across.
* [[ESO 383-76]], one of the [[List of largest galaxies|largest known galaxies]], has a diameter of {{Convert|540.9|kpc|e6ly|1|abbr=unit}}.
* The [[Andromeda Galaxy]] ([[Messier object|M31]]) is about {{Convert|780|kpc|e6ly|abbr=unit}} away from the Earth.
* The [[Andromeda Galaxy]] ([[Messier object|M31]]) is about {{Convert|780|kpc|e6ly|abbr=unit}} away from the Earth.


=== Megaparsecs and gigaparsecs ===
=== Megaparsecs and gigaparsecs ===
<!-- Template:Convert/Mpc & Template:Convert/Gpc link here. -->
<!-- Template:Convert/Mpc & Template:Convert/Gpc link here. -->
Astronomers typically express the distances between neighbouring galaxies and [[galaxy cluster]]s in megaparsecs (Mpc). A megaparsec is one million parsecs, or about 3,260,000 light years.<ref>{{cite web |url=https://astronomy.com/magazine/ask-astro/2020/02/why-is-a-parsec-326-light-years |title=Why is a parsec 3.26 light-years? |website=Astronomy.com |date=1 February 2020 |access-date=20 July 2021 |url-status=live}}</ref> Sometimes, galactic distances are given in units of Mpc/''h'' (as in "50/''h''&nbsp;Mpc", also written "{{nowrap|50 Mpc ''h''<sup>−1</sup>}}"). ''h'' is a constant (the "[[dimensionless Hubble constant]]") in the range {{nowrap|0.5 < ''h'' < 0.75}} reflecting the uncertainty in the value of the [[Hubble constant]] ''H'' for the rate of expansion of the universe: {{nowrap|1=''h'' = {{sfrac|''H''|100&nbsp;(km/s)/Mpc}}}}. The Hubble constant becomes relevant when converting an observed [[redshift]] ''z'' into a distance ''d'' using the formula {{nowrap|''d'' ≈ {{sfrac|''[[Speed of light|c]]''|''H''}} × ''z''}}.<ref>{{Cite web |title=Galaxy structures: the large scale structure of the nearby universe |url=http://pil.phys.uniroma1.it/twiki/bin/view/Pil/GalaxyStructures |url-status=dead |archive-url=https://web.archive.org/web/20070305202144/http://pil.phys.uniroma1.it/twiki/bin/view/Pil/GalaxyStructures |archive-date=5 March 2007 |access-date=22 May 2007}}</ref>
Astronomers typically express the distances between neighbouring galaxies and [[galaxy cluster]]s in megaparsecs (Mpc). A megaparsec is one million parsecs, or about 3,260,000 light years.<ref>{{cite web |url=https://astronomy.com/magazine/ask-astro/2020/02/why-is-a-parsec-326-light-years |title=Why is a parsec 3.26 light-years? |website=Astronomy.com |date=1 February 2020 |access-date=20 July 2021 }}</ref> Sometimes, galactic distances are given in units of Mpc/''h'' (as in "50/''h''&nbsp;Mpc", also written "{{nowrap|50 Mpc ''h''<sup>−1</sup>}}"). ''h'' is a constant (the "[[dimensionless Hubble constant]]") in the range {{nowrap|0.5 < ''h'' < 0.75}} reflecting the uncertainty in the value of the [[Hubble constant]] ''H'' for the rate of expansion of the universe: {{nowrap|1=''h'' = {{sfrac|''H''|100&nbsp;(km/s)/Mpc}}}}. The Hubble constant becomes relevant when converting an observed [[redshift]] ''z'' into a distance ''d'' using the formula {{nowrap|''d'' ≈ {{sfrac|''[[Speed of light|c]]''|''H''}} × ''z''}}.<ref>{{Cite web |title=Galaxy structures: the large scale structure of the nearby universe |url=http://pil.phys.uniroma1.it/twiki/bin/view/Pil/GalaxyStructures |url-status=dead |archive-url=https://web.archive.org/web/20070305202144/http://pil.phys.uniroma1.it/twiki/bin/view/Pil/GalaxyStructures |archive-date=5 March 2007 |access-date=22 May 2007}}</ref>


One gigaparsec (Gpc) is [[1000000000 (number)|one billion]] parsecs — one of the largest [[Orders of magnitude (length)|units of length]] commonly used. One gigaparsec is about {{Convert|1|Gpc|e9ly|sigfig=3|abbr=unit|disp=out}}, or roughly {{sfrac|14}} of the distance to the [[Cosmological horizon#Practical horizons|horizon]] of the [[observable universe]] (dictated by the [[cosmic background radiation]]). Astronomers typically use gigaparsecs to express the sizes of [[Large-scale structure of the cosmos|large-scale structures]] such as the size of, and distance to, the [[CfA2 Great Wall]]; the distances between galaxy clusters; and the distance to [[quasar]]s.
One gigaparsec (Gpc) is [[1000000000 (number)|one billion]] parsecs — one of the largest [[Orders of magnitude (length)|units of length]] commonly used. One gigaparsec is about {{Convert|1|Gpc|e9ly|sigfig=3|abbr=unit|disp=out}}, or roughly {{sfrac|14}} of the distance to the [[Cosmological horizon#Practical horizons|horizon]] of the [[observable universe]] (dictated by the [[cosmic microwave background radiation]]). Astronomers typically use gigaparsecs to express the sizes of [[Large-scale structure of the cosmos|large-scale structures]] such as the size of, and distance to, the [[CfA2 Great Wall]]; the distances between galaxy clusters; and the distance to [[quasar]]s.


For example:
For example:
Line 142: Line 141:


The observational volume of gravitational wave interferometers (e.g., [[LIGO]], [[Virgo interferometer|Virgo]]) is stated in terms of cubic megaparsecs{{efn|name=vol}} (Mpc<sup>3</sup>) and is essentially the value of the effective distance cubed.
The observational volume of gravitational wave interferometers (e.g., [[LIGO]], [[Virgo interferometer|Virgo]]) is stated in terms of cubic megaparsecs{{efn|name=vol}} (Mpc<sup>3</sup>) and is essentially the value of the effective distance cubed.

==In popular culture==
The parsec was seemingly used incorrectly as a measurement of time by [[Han Solo]] in the first ''[[A New Hope|Star Wars]]'' film, when he claimed his ship, the ''[[Millennium Falcon]]'' "made the [[Kessel Run]] in less than 12 parsecs". The claim was repeated in ''[[Star Wars: The Force Awakens|The Force Awakens]]'', but this was clarified in ''[[Solo: A Star Wars Story]]'', by stating the ''[[Millennium Falcon]]'' traveled a shorter distance (as opposed to a quicker time) due to a more dangerous route through the Kessel Run, enabled by its speed and maneuverability.<ref>{{Cite web |date=30 May 2018 |title='Solo' Corrected One of the Most Infamous 'Star Wars' Plot Holes |url=https://www.esquire.com/entertainment/movies/a20967903/solo-star-wars-kessel-distance-plot-hole/ |website=Esquire}}</ref> It is also used ambiguously as a spatial unit in ''[[The Mandalorian]]''.<ref>{{Cite web |last=Choi |first=Charlse |date=5 November 2019 |title='Star Wars' Gets the Parsec Wrong Again in 'The Mandalorian' |url=https://www.space.com/star-wars-the-mandalorian-parsec.html |access-date=6 May 2020 |website=space.com}}</ref>

In the book ''[[A Wrinkle in Time]]'', "Megaparsec" is Mr. Murry's nickname for his daughter Meg.<ref>{{Cite web |title=In "A Wrinkle in Time," what is Mr. Murry's nickname for Meg? |url=https://www.enotes.com/homework-help/wrinkle-time-what-mr-murrays-nickname-for-meg-39431b |access-date=6 May 2020}}</ref>


==See also==
==See also==

Latest revision as of 17:43, 14 December 2024

Parsec
A parsec is the distance from the Sun to an astronomical object that has a parallax angle of one arcsecond (not to scale)
General information
Unit systemastronomical units
Unit oflength/distance
Symbolpc
Conversions
1 pc in ...... is equal to ...
   metric (SI) units   3.0857×1016 m
   ≈31 petametres
   imperial  US units   1.9174×1013 mi
   astronomical units   206,265 au
   3.26156 ly

The parsec (symbol: pc) is a unit of length used to measure the large distances to astronomical objects outside the Solar System, approximately equal to 3.26 light-years or 206,265 astronomical units (AU), i.e. 30.9 trillion kilometres (19.2 trillion miles).[a] The parsec unit is obtained by the use of parallax and trigonometry, and is defined as the distance at which 1 AU subtends an angle of one arcsecond[1] (1/3600 of a degree). The nearest star, Proxima Centauri, is about 1.3 parsecs (4.2 light-years) from the Sun: from that distance, the gap between the Earth and the Sun spans slightly less than 1/3600 of one degree of view.[2] Most stars visible to the naked eye are within a few hundred parsecs of the Sun, with the most distant at a few thousand parsecs, and the Andromeda Galaxy at over 700,000 parsecs.[3]

The word parsec is a portmanteau of "parallax of one second" and was coined by the British astronomer Herbert Hall Turner in 1913[4] to simplify astronomers' calculations of astronomical distances from only raw observational data. Partly for this reason, it is the unit preferred in astronomy and astrophysics, though the light-year remains prominent in popular science texts and common usage. Although parsecs are used for the shorter distances within the Milky Way, multiples of parsecs are required for the larger scales in the universe, including kiloparsecs (kpc) for the more distant objects within and around the Milky Way, megaparsecs (Mpc) for mid-distance galaxies, and gigaparsecs (Gpc) for many quasars and the most distant galaxies.

In August 2015, the International Astronomical Union (IAU) passed Resolution B2 which, as part of the definition of a standardized absolute and apparent bolometric magnitude scale, mentioned an existing explicit definition of the parsec as exactly 648000/π au, or approximately 3.0856775814913673×1016 metres (based on the IAU 2012 definition of the astronomical unit). This corresponds to the small-angle definition of the parsec found in many astronomical references.[5][6]

History and derivation

[edit]

Imagining an elongated right triangle in space, where the shorter leg measures one au (astronomical unit, the average EarthSun distance) and the subtended angle of the vertex opposite that leg measures one arcsecond (13600 of a degree), the parsec is defined as the length of the adjacent leg. The value of a parsec can be derived through the rules of trigonometry. The distance from Earth whereupon the radius of its solar orbit subtends one arcsecond.

One of the oldest methods used by astronomers to calculate the distance to a star is to record the difference in angle between two measurements of the position of the star in the sky. The first measurement is taken from the Earth on one side of the Sun, and the second is taken approximately half a year later, when the Earth is on the opposite side of the Sun.[b] The distance between the two positions of the Earth when the two measurements were taken is twice the distance between the Earth and the Sun. The difference in angle between the two measurements is twice the parallax angle, which is formed by lines from the Sun and Earth to the star at the distant vertex. Then the distance to the star could be calculated using trigonometry.[7] The first successful published direct measurements of an object at interstellar distances were undertaken by German astronomer Friedrich Wilhelm Bessel in 1838, who used this approach to calculate the 3.5-parsec distance of 61 Cygni.[8]

Diagrams illustrating the apparent change in position of a celestial object when viewed from different positions in Earth's orbit.
Stellar parallax motion from annual parallax

The parallax of a star is defined as half of the angular distance that a star appears to move relative to the celestial sphere as Earth orbits the Sun. Equivalently, it is the subtended angle, from that star's perspective, of the semimajor axis of the Earth's orbit. Substituting the star's parallax for the one arcsecond angle in the imaginary right triangle, the long leg of the triangle will measure the distance from the Sun to the star. A parsec can be defined as the length of the right triangle side adjacent to the vertex occupied by a star whose parallax angle is one arcsecond.

The use of the parsec as a unit of distance follows naturally from Bessel's method, because the distance in parsecs can be computed simply as the reciprocal of the parallax angle in arcseconds (i.e.: if the parallax angle is 1 arcsecond, the object is 1 pc from the Sun; if the parallax angle is 0.5 arcseconds, the object is 2 pc away; etc.). No trigonometric functions are required in this relationship because the very small angles involved mean that the approximate solution of the skinny triangle can be applied.

Though it may have been used before, the term parsec was first mentioned in an astronomical publication in 1913. Astronomer Royal Frank Watson Dyson expressed his concern for the need of a name for that unit of distance. He proposed the name astron, but mentioned that Carl Charlier had suggested siriometer and Herbert Hall Turner had proposed parsec.[4] It was Turner's proposal that stuck.

Calculating the value of a parsec

[edit]

By the 2015 definition, 1 au of arc length subtends an angle of 1″ at the center of the circle of radius 1 pc. That is, 1 pc = 1 au/tan(1″) ≈ 206,264.8 au by definition.[9] Converting from degree/minute/second units to radians,

, and
(exact by the 2012 definition of the au)

Therefore, (exact by the 2015 definition)

Therefore,

(to the nearest metre).

Approximately,

Diagram of parsec.

In the diagram above (not to scale), S represents the Sun, and E the Earth at one point in its orbit (such as to form a right angle at S[b]). Thus the distance ES is one astronomical unit (au). The angle SDE is one arcsecond (1/3600 of a degree) so by definition D is a point in space at a distance of one parsec from the Sun. Through trigonometry, the distance SD is calculated as follows:

Because the astronomical unit is defined to be 149597870700 m,[10] the following can be calculated:

Therefore, 1 parsec 206264.806247096 astronomical units
3.085677581×1016 metres
30.856775815 trillion kilometres
19.173511577 trillion miles

Therefore, if ly ≈ 9.46×1015 m,

Then 1 pc3.261563777 ly

A corollary states that a parsec is also the distance from which a disc that is one au in diameter must be viewed for it to have an angular diameter of one arcsecond (by placing the observer at D and a disc spanning ES).

Mathematically, to calculate distance, given obtained angular measurements from instruments in arcseconds, the formula would be:

where θ is the measured angle in arcseconds, Distanceearth-sun is a constant (1 au or 1.5813×10−5 ly). The calculated stellar distance will be in the same measurement unit as used in Distanceearth-sun (e.g. if Distanceearth-sun = 1 au, unit for Distancestar is in astronomical units; if Distanceearth-sun = 1.5813×10−5 ly, unit for Distancestar is in light-years).

The length of the parsec used in IAU 2015 Resolution B2[11] (exactly 648000/π astronomical units) corresponds exactly to that derived using the small-angle calculation. This differs from the classic inverse-tangent definition by about 200 km, i.e.: only after the 11th significant figure. As the astronomical unit was defined by the IAU (2012) as an exact length in metres, so now the parsec corresponds to an exact length in metres. To the nearest meter, the small-angle parsec corresponds to 30856775814913673 m.

Usage and measurement

[edit]

The parallax method is the fundamental calibration step for distance determination in astrophysics; however, the accuracy of ground-based telescope measurements of parallax angle is limited to about 0.01″, and thus to stars no more than 100 pc distant.[12] This is because the Earth's atmosphere limits the sharpness of a star's image.[citation needed] Space-based telescopes are not limited by this effect and can accurately measure distances to objects beyond the limit of ground-based observations. Between 1989 and 1993, the Hipparcos satellite, launched by the European Space Agency (ESA), measured parallaxes for about 100000 stars with an astrometric precision of about 0.97 mas, and obtained accurate measurements for stellar distances of stars up to 1000 pc away.[13][14]

ESA's Gaia satellite, which launched on 19 December 2013, is intended to measure one billion stellar distances to within 20 microarcseconds, producing errors of 10% in measurements as far as the Galactic Centre, about 8000 pc away in the constellation of Sagittarius.[15]

Distances in parsecs

[edit]

Distances less than a parsec

[edit]

Distances expressed in fractions of a parsec usually involve objects within a single star system. So, for example:

  • One astronomical unit (au), the distance from the Sun to the Earth, is just under 5×10−6 pc.
  • The most distant space probe, Voyager 1, was 0.0007897 pc from Earth as of February 2024. Voyager 1 took 46 years to cover that distance.
  • The Oort cloud is estimated to be approximately 0.6 pc in diameter
As observed by the Hubble Space Telescope, the astrophysical jet erupting from the active galactic nucleus of M87 subtends 20″ and is thought to be 1.5 kiloparsecs (4,892 ly) long (the jet is somewhat foreshortened from Earth's perspective).

Parsecs and kiloparsecs

[edit]

Distances expressed in parsecs (pc) include distances between nearby stars, such as those in the same spiral arm or globular cluster. A distance of 1,000 parsecs (3,262 ly) is denoted by the kiloparsec (kpc). Astronomers typically use kiloparsecs to express distances between parts of a galaxy or within groups of galaxies. So, for example :

  • Proxima Centauri, the nearest known star to Earth other than the Sun, is about 1.3 parsecs (4.24 ly) away by direct parallax measurement.
  • The distance to the open cluster Pleiades is 130±10 pc (420±30 ly) from us per Hipparcos parallax measurement.
  • The centre of the Milky Way is more than 8 kiloparsecs (26,000 ly) from the Earth and the Milky Way is roughly 34 kiloparsecs (110,000 ly) across.
  • ESO 383-76, one of the largest known galaxies, has a diameter of 540.9 kpc (1.8 million ly).
  • The Andromeda Galaxy (M31) is about 780 kpc (2.5 million ly) away from the Earth.

Megaparsecs and gigaparsecs

[edit]

Astronomers typically express the distances between neighbouring galaxies and galaxy clusters in megaparsecs (Mpc). A megaparsec is one million parsecs, or about 3,260,000 light years.[16] Sometimes, galactic distances are given in units of Mpc/h (as in "50/h Mpc", also written "50 Mpc h−1"). h is a constant (the "dimensionless Hubble constant") in the range 0.5 < h < 0.75 reflecting the uncertainty in the value of the Hubble constant H for the rate of expansion of the universe: h = H/100 (km/s)/Mpc. The Hubble constant becomes relevant when converting an observed redshift z into a distance d using the formula dc/H × z.[17]

One gigaparsec (Gpc) is one billion parsecs — one of the largest units of length commonly used. One gigaparsec is about 3.26 billion ly, or roughly 1/14 of the distance to the horizon of the observable universe (dictated by the cosmic microwave background radiation). Astronomers typically use gigaparsecs to express the sizes of large-scale structures such as the size of, and distance to, the CfA2 Great Wall; the distances between galaxy clusters; and the distance to quasars.

For example:

Volume units

[edit]

To determine the number of stars in the Milky Way, volumes in cubic kiloparsecs[c] (kpc3) are selected in various directions. All the stars in these volumes are counted and the total number of stars statistically determined. The number of globular clusters, dust clouds, and interstellar gas is determined in a similar fashion. To determine the number of galaxies in superclusters, volumes in cubic megaparsecs[c] (Mpc3) are selected. All the galaxies in these volumes are classified and tallied. The total number of galaxies can then be determined statistically. The huge Boötes void is measured in cubic megaparsecs.[20]

In physical cosmology, volumes of cubic gigaparsecs[c] (Gpc3) are selected to determine the distribution of matter in the visible universe and to determine the number of galaxies and quasars. The Sun is currently the only star in its cubic parsec,[c] (pc3) but in globular clusters the stellar density could be from 100–1000 pc−3.

The observational volume of gravitational wave interferometers (e.g., LIGO, Virgo) is stated in terms of cubic megaparsecs[c] (Mpc3) and is essentially the value of the effective distance cubed.

See also

[edit]

Notes

[edit]
  1. ^ One trillion here is short scale, ie. 1012 (one million million, or billion in long scale).
  2. ^ a b Terrestrial observations of a star's position should be taken when the Earth is at the furthest points in its orbit from a line between the Sun and the star, in order to form a right angle at the Sun and a full au of separation as viewed from the star.
  3. ^ a b c d e
    1 pc3 2.938×1049 m3
    1 kpc32.938×1058 m3
    1 Mpc32.938×1067 m3
    1 Gpc32.938×1076 m3
    1 Tpc32.938×1085 m3

References

[edit]
  1. ^ "Cosmic Distance Scales – The Milky Way". Retrieved 24 September 2014.
  2. ^ Benedict, G. F.; et al. "Astrometric Stability and Precision of Fine Guidance Sensor #3: The Parallax and Proper Motion of Proxima Centauri" (PDF). Proceedings of the HST Calibration Workshop. pp. 380–384. Retrieved 11 July 2007.
  3. ^ "Farthest Stars". StarDate. University of Texas at Austin. 15 May 2021. Retrieved 5 September 2021.
  4. ^ a b Dyson, F. W. (March 1913). "The distribution in space of the stars in Carrington's Circumpolar Catalogue". Monthly Notices of the Royal Astronomical Society. 73 (5): 342. Bibcode:1913MNRAS..73..334D. doi:10.1093/mnras/73.5.334. [paragraph 14, page 342] Taking the unit of distance R* to be that corresponding to a parallax of 1″·0 [… Footnote:]
    * There is need for a name for this unit of distance. Mr. Charlier has suggested Siriometer, but if the violence to the Greek language can be overlooked, the word Astron might be adopted. Professor Turner suggests Parsec, which may be taken as an abbreviated form of "a distance corresponding to a parallax of one second".
  5. ^ Cox, Arthur N., ed. (2000). Allen's Astrophysical Quantities (4th ed.). New York: AIP Press / Springer. Bibcode:2000asqu.book.....C. ISBN 978-0387987460.
  6. ^ Binney, James; Tremaine, Scott (2008). Galactic Dynamics (2nd ed.). Princeton, NJ: Princeton University Press. Bibcode:2008gady.book.....B. ISBN 978-0-691-13026-2.
  7. ^ High Energy Astrophysics Science Archive Research Center (HEASARC). "Deriving the Parallax Formula". NASA's Imagine the Universe!. Astrophysics Science Division (ASD) at NASA's Goddard Space Flight Center. Retrieved 26 November 2011.
  8. ^ Bessel, F. W. (1838). "Bestimmung der Entfernung des 61sten Sterns des Schwans" [Determination of the distance of the 61st star of Cygnus]. Astronomische Nachrichten. 16 (5): 65–96. Bibcode:1838AN.....16...65B. doi:10.1002/asna.18390160502.
  9. ^ B. Luque; F. J. Ballesteros (2019). "Title: To the Sun and beyond". Nature Physics. 15 (12): 1302. Bibcode:2019NatPh..15.1302L. doi:10.1038/s41567-019-0685-3.
  10. ^ International Astronomical Union, ed. (31 August 2012), "RESOLUTION B2 on the re-definition of the astronomical unit of length" (PDF), RESOLUTION B2, Beijing: International Astronomical Union, The XXVIII General Assembly of the International Astronomical Union recommends [adopted] that the astronomical unit be redefined to be a conventional unit of length equal to exactly 149597870700 m, in agreement with the value adopted in IAU 2009 Resolution B2
  11. ^ International Astronomical Union, ed. (13 August 2015), "RESOLUTION B2 on recommended zero points for the absolute and apparent bolometric magnitude scales" (PDF), RESOLUTION B2, Honolulu: International Astronomical Union, The XXIX General Assembly of the International Astronomical Union notes [4] that the parsec is defined as exactly (648 000/) au per the AU definition in IAU 2012 Resolution B2
  12. ^ Pogge, Richard. "Astronomy 162". Ohio State University.
  13. ^ "The Hipparcos Space Astrometry Mission". Retrieved 28 August 2007.
  14. ^ Turon, Catherine. "From Hipparchus to Hipparcos".
  15. ^ "GAIA". European Space Agency.
  16. ^ "Why is a parsec 3.26 light-years?". Astronomy.com. 1 February 2020. Retrieved 20 July 2021.
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