The parsec (symbol: pc) is a unit of length used in astronomy, equal to about 3.26 light-years, or about 30.9 trillion kilometres (19.2 trillion miles).
The name parsec is "an abbreviated form of 'a distance corresponding to a parallax of one arcsecond'."^{[1]} It was coined in 1913 at the suggestion of British astronomer Herbert Hall Turner. A parsec is the distance from the Sun to an astronomical object which has a parallax angle of one arcsecond (^{1}⁄_{3,600} of a degree). In other words, imagine three straight lines forming a right triangle between the Earth, the Sun and a distant object, as follows: line 1 connects the Earth and the Sun, line 2, perpendicular to the first line, connects the Sun and the object, and line 3 connects the object to the Earth. Now, if the angle at the object between lines 2 and 3 is exactly one arcsecond, then the object's distance from the Sun would be exactly one parsec.
An object's distance in parsecs is numerically (though not dimensionally because they are measures of distance and angle, respectively) equal to the reciprocal of half the number of arcseconds by which its position appears to change when observed for six months because Earth moves to the other side of its orbit and is therefore twice the base of the aforementioned triangle away from where it was before ($d\; (\backslash mathrm\{pc\})\; =\; 1\; /\; .5p\; (\backslash mathrm\{arcsec\})\; =\; 2\; /\; p(\backslash mathrm\{arcsec\})$ ).^{[2]} The less an object appears to have moved, the further it is from the Sun, and vice versa because the relationship between the distance to the object and the magnitude of its parallax is an inverse one: the shorter the distance, the greater the parallax angle.
Parsecs remain in common use in contemporary astrophysics, even though the actual parallax shift for objects at cosmological distances is unmeasurable. The use of light-years is common only in popular science texts, although light travel time is sometimes used to relate distances in small astrophysical systems where radiation processes can play a major role.
Equivalencies in other units
1 parsec ≡ 648000 / Template:Pi astronomical units
- ≈ 206264.81 astronomical units
- ≈ 30856776 million kilometres
- ≈ 19173512 million miles
- ≈ 3.2615638 light years
History and derivation
The parsec is equal to the length of the adjacent side of an imaginary right triangle in space. The two dimensions on which this triangle is based are the angle (which is defined as 1 arcsecond), and the opposite side (which is defined as 1 astronomical unit, which is the average distance from the Earth to the Sun). Using these two measurements, along with the rules of trigonometry, the length of the adjacent side (the parsec) can be found.
One of the oldest methods for astronomers to calculate the distance to a star was to record the difference in angle between two measurements of the position of the star in the sky. The first measurement was taken from the Earth on one side of the Sun, and the second was taken half a year later when the Earth was on the opposite side of the Sun. The distance between the two positions of the Earth when the two measurements were taken was known to be twice the distance between the Earth and the Sun. The difference in angle between the two measurements was known to be twice the parallax angle, which is formed by lines from the Sun and Earth to the star at the vertex. Then the distance to the star could be calculated using trigonometry.^{[3]} The first successful 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 three and a half parsec distance of 61 Cygni.^{[4]}
The parallax of a star is taken to be 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 semi-major axis of 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 1 astronomical unit (AU)), and the length of the 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 adjacent side of this right triangle in space when the parallax angle is 1 arcsecond.
The use of the parsec as a unit of distance follows naturally from Bessel's method, since 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 arcsecond, 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.^{[5]} It was Turner's proposal that stuck.
Calculating the value of a 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 (1/3600 of a degree) so by definition D is a point in space at a distance of one parsec from the Sun. By trigonometry, the distance SD is
- $SD\; =\; \backslash frac\{\backslash mathrm\{ES\}\}\{\backslash tan\; 1^\{\backslash prime\backslash prime\}\}$
Using the small-angle approximation, by which the sine (and, hence, the tangent) of an extremely small angle is essentially equal to the angle itself (in radians),
- $SD\; \backslash approx\; \backslash frac\{\backslash mathrm\{ES\}\}\{1^\{\backslash prime\backslash prime\}\}\; =\; \backslash frac\{1\; \backslash ,\; \backslash mbox\{AU\}\}\{(\backslash tfrac\{1\}\{60\; \backslash times\; 60\}\; \backslash times\; \backslash tfrac\{\backslash pi\}\{180\})\}\; =\; \backslash frac\{648\backslash ,000\}\{\backslash pi\}\; \backslash ,\; \backslash mbox\{AU\}\; \backslash approx\; 206\backslash ,264.81\; \backslash mbox\{\; AU\}\; .$
One AU ≈ 149597870700 metres, so 1 parsec ≈ 3.085678×10^{16} m ≈ 3.261564 light-years.
A corollary is that 1 parsec is also the distance from which a disc with a diameter of 1 AU must be viewed for it to have an angular diameter of 1 arcsecond (by placing the observer at D and a diameter of the disc on ES).
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 0.01 arcseconds, and thus to stars no more than 100 pc distant.^{[6]} This is because the Earth’s atmosphere limits the sharpness of a star's image.^{[7]} 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 100,000 stars with an astrometric precision of about 0.97 milliarcseconds, and obtained accurate measurements for stellar distances of stars up to 1,000 pc away.^{[8]}^{[9]}
NASA's FAME satellite was to have been launched in 2004, to measure parallaxes for about 40 million stars with sufficient precision to measure stellar distances of up to 2,000 pc. However, the mission's funding was withdrawn by NASA in January 2002.^{[10]} ESA's Gaia satellite, which was due to be launched in late 2012, but has been pushed to August 2013, is intended to measure one billion stellar distances to within 20 microarcseconds, producing errors of 10% in measurements as far as the Galactic Center, about 8,000 pc away in the constellation of Sagittarius.^{[11]}
Distances in parsecs
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 0.000005 parsecs (150,000,000 km; 96,000,000 mi).
- The most distant space probe, Voyager 1, was 0.0006 parsecs (0.002 light-years) from Earth as of May 2013^{[update]}. It took Voyager 35 years to cover that distance.
- The Oort cloud is estimated to be approximately 0.6 parsecs (2.0 light-years) in diameter
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 1,000 parsecs (3,262 light-years) is commonly 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:
- One parsec is approximately 3.26 light-years.
- The nearest known star to the Earth, other than the Sun, Proxima Centauri, is 1.30 parsecs (4.24 light-years) away, by direct parallax measurement.
- The distance to the open cluster Pleiades is 130 ± 10 pc (420 ± 32.6 light-years) from us, per Hipparcos parallax measurement.
- The center of the Milky Way is more than 8 kiloparsecs (26,000 light-years) from the Earth, and the Milky Way is roughly 34 kpc (110,000 light-years) across.
- The Andromeda Galaxy (M31) is ~780 kpc (~2.5 million light-years) away from the Earth.
Megaparsecs and gigaparsecs
A distance of one million parsecs (3.26 million light-years or 3.26 "Mly") is commonly denoted by the megaparsec (Mpc). Astronomers typically express the distances between neighbouring galaxies and galaxy clusters in megaparsecs.
Galactic distances are sometimes given in units of Mpc/h (as in "50/h Mpc"). h is a parameter in the range [0.5,0.75] 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 d ≈ (c / H) × z.^{[12]}
One gigaparsec (Gpc) is one billion parsecs — one of the largest units of length commonly used. One gigaparsec is about 3.26 billion light-years (3.26 "Gly"), or roughly one fourteenth of the distance to the horizon of the observable universe (dictated by the cosmic 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
To determine the number of stars in the Milky Way Galaxy, volumes in cubic kiloparsecsTemplate:Efn (kpc^{3}) 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 megaparsecsTemplate:Efn (Mpc^{3}) are selected. All the galaxies in these volumes are classified and tallied. The total number of galaxies can then be determined statistically. The huge void in Boötes^{[15]} is measured in cubic megaparsecs.
In cosmology, volumes of cubic gigaparsecsTemplate:Efn (Gpc^{3}) are selected to determine the distribution of matter in the visible universe and to determine the number of galaxies and quasars. The Sun is alone in its cubic parsec,Template:Efn (pc^{3}) but in globular clusters the stellar density per cubic parsec could be from 100 to 1,000.
References
Explanatory notes
Template:Notes
Citations
External links
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