Parsec

 ( Units Of Length ) 

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 or (AU), i.e. . The parsec unit is obtained by the use of parallax and trigonometry, and is defined as the distance at which 1 AU subtended angle an angle of one arcsecond ( of a degree). The nearest star, Proxima Centauri, is about from the Sun: from that distance, the gap between the Earth and the Sun spans slightly less than one arcsecond. Most Naked-eye stars 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.

The word parsec is a shortened form of a distance corresponding to a parallax of one second, coined by the British astronomer Herbert Hall Turner in 1913. The unit was introduced to simplify the calculation of astronomical distances from raw observational data. Partly for this reason, it is the unit preferred in astronomy and astrophysics, though in popular science texts and common usage the light-year remains prominent. 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-parsecs (kpc) for the more distant objects within and around the Milky Way, Mega-parsecs (Mpc) for mid-distance galaxies, and giga-parsecs (Gpc) for many 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  au, or approximately  metres, given the IAU 2012 exact definition of the astronomical unit in metres. This corresponds to the small-angle definition of the parsec found in many astronomical references.

(2025). 9780691130262, Princeton University Press. ISBN 9780691130262

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History and derivation Imagining an elongated right triangle in space, where the shorter leg measures one au (astronomical unit, the average Earth–Sun distance) and the subtended of the vertex opposite that leg measures one arcsecond ( 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. 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. 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.

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. It was Turner's proposal that stuck.

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

$\backslash frac\{1\; \backslash text\{\; pc\}\}\{1\; \backslash text\{\; au\}\}\; =\; \backslash frac\{180\; \backslash times\; 60\; \backslash times\; 60\}\{\backslash pi\}$, and

$1\; \backslash text\{\; au\}\; =\; 149\backslash ,597\backslash ,870\backslash ,700\; \backslash text\{\; m\}$ (exact by the 2012 definition of the au)

Therefore, $$\backslash pi\; ~\; \backslash mathrm\{pc\}\; =\; 180\; \backslash times\; 60\; \backslash times\; 60\; ~\; \backslash mathrm\{au\}\; =\; 180\; \backslash times\; 60\; \backslash times\; 60\; \backslash times\; 149\backslash ,597\backslash ,870\backslash ,700\; ~\; \backslash mathrm\{m\}\; =\; 96\backslash ,939\backslash ,420\backslash ,213\backslash ,600\backslash ,000\; ~\; \backslash mathrm\{m\}$$ (exact by the 2015 definition)

Therefore,

$$1\; ~\; \backslash mathrm\{pc\}\; =\; \backslash frac\{96\backslash ,939\backslash ,420\backslash ,213\backslash ,600\backslash ,000\}\{\backslash pi\}\; ~\; \backslash mathrm\{m\}\; =\; 30\backslash ,856\backslash ,775\backslash ,814\backslash ,913\backslash ,673\; ~\; \backslash mathrm\{m\}$$ (to the nearest metre).

Approximately,

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). Thus the distance ES is one astronomical unit (au). The angle SDE is one arcsecond ( 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 , the following can be calculated:

Therefore, 1 parsec	≈ astronomical units
	≈ metres
	≈  trillion
	≈  trillion

Therefore, if ≈ ,

Then ≈

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:

$$\backslash text\{Distance\}\_\backslash text\{star\}\; =\; \backslash frac\; \{\backslash text\{Distance\}\_\backslash text\{earth-sun\}\}\{\backslash tan\{\backslash frac\{\backslash theta\}\{3600\}\}\}$$

where θ is the measured angle in arcseconds, Distance_earth-sun is a constant ( or ). The calculated stellar distance will be in the same measurement unit as used in Distance_earth-sun (e.g. if Distance_earth-sun = , unit for Distance_star is in astronomical units; if Distance_earth-sun = , unit for Distance_star is in light-years).

The length of the parsec used in IAU 2015 Resolution B2 (exactly astronomical units) corresponds exactly to that derived using the small-angle calculation. This differs from the classic inverse-tangent definition by about , 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 metre, the small-angle parsec corresponds to .

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Usage and measurement 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 , and thus to stars no more than distant. This is because the Earth's atmosphere limits the sharpness of a star's image. 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 stars with an astrometry precision of about , and obtained accurate measurements for stellar distances of stars up to away.

ESA's Gaia mission, which launched on 19 December 2013, gathered data with a goal of measuring one billion stellar distances to within s, producing errors of 10% in measurements as far as the Galactic Center, about away in the constellation of Sagittarius.

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Distances in parsecs

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Distances less than a parsec 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 .
• The most distant space probe, Voyager 1, was from Earth . Voyager 1 took to cover that distance.
• The Oort cloud is estimated to be approximately in diameter

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

• Proxima Centauri, the nearest known star to Earth other than the Sun, is about away by direct parallax measurement.
• The distance to the open cluster Pleiades is () from us per Hipparcos parallax measurement.
• The Galactic Center of the Milky Way is more than from the Earth and the Milky Way is roughly across.
• ESO 383-76, one of the largest known galaxies, has a diameter of .
• The Andromeda Galaxy (Messier object) is about away from the Earth.

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Megaparsecs and gigaparsecs Astronomers typically express the distances between neighbouring galaxies and in megaparsecs (Mpc). A megaparsec is one million parsecs, or about 3,260,000 light years. Sometimes, galactic distances are given in units of Mpc/ h (as in "50/ h Mpc", also written ""). h is a constant (the "dimensionless Hubble constant") in the range reflecting the uncertainty in the value of the Hubble constant H for the rate of expansion of the universe: . The Hubble constant becomes relevant when converting an observed redshift z into a distance d using the formula .

One gigaparsec (Gpc) is one billion parsecs — one of the largest units of length commonly used. One gigaparsec is about , or roughly 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 .

For example:

• The Andromeda Galaxy is about from the Earth.
• The nearest large galaxy cluster, the Virgo Cluster, is about from the Earth.
• The galaxy RXJ1242-11, observed to have a supermassive black hole core similar to the Milky Way's, is about from the Earth.
• The galaxy filament Hercules–Corona Borealis Great Wall, which is since November 2013 the largest known structure in the universe, is about across.
• The particle horizon (the boundary of the observable universe) has a radius of about .

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Volume units To determine the number of stars in the Milky Way, volumes in cubic kiloparsecs (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 , volumes in cubic megaparsecs (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.

In physical cosmology, volumes of cubic gigaparsecs (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, (pc³) but in globular clusters the stellar density could be from .

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

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See also

• Attoparsec
• Distance measure

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In popular culture The parsec is used incorrectly as a measurement of time by Han Solo in the first Star Wars film, when he claims his ship, the Millennium Falcon "made the Kessel Run in less than 12 parsecs," originally with the intention of presenting Solo as "something of a bull artist who didn't always know precisely what he was talking about." The claim is repeated in , but in it is stated that the Millennium Falcon has 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. It is also used incorrectly in The Mandalorian.

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Notes

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External links

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