**Stellar parallax** is the apparent shift of position of any nearby star (or other object) against the background of distant objects. Created by the different orbital positions of Earth, the extremely small observed shift is largest at time intervals of about six months, when Earth arrives at opposite sides of the Sun in its orbit, giving a baseline distance of about two astronomical units between observations. The parallax itself is considered to be half of this maximum, about equivalent to the observational shift that would occur due to the different positions of Earth and the Sun, a baseline of one astronomical unit (AU).

Stellar parallax is so difficult to detect that its existence was the subject of much debate in astronomy for hundreds of years. Friedrich Bessel made the first successful parallax measurement in 1838, for the star 61 Cygni, using a Fraunhofer heliometer at Königsberg Observatory.

## Parallax method

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Throughout the year the position of a star S is noted in relation to other stars in its apparent neighborhood:

Stars that did not seem to move in relation to each other are used as reference points to determine the path of S.

The observed path is an ellipse: the projection of Earth’s orbit around the Sun through S onto the distant background of non-moving stars. The farther S is removed from Earth’s orbital axis, the greater the eccentricity of the path of S. The center of the ellipse corresponds to the point where S would be seen from the Sun:

The plane of Earth’s orbit is at an angle to a line from the Sun through S. The vertices v and v' of the elliptical projection of the path of S are projections of positions of Earth E and E’ such that a line E-E’ intersects the line Sun-S at a right angle; the triangle created by points E, E’ and S is an isosceles triangle with the line Sun-S as its symmetry axis.

Any stars that did not move between observations are, for the purpose of the accuracy of the measurement, infinitely far away. This means that the distance of the movement of the Earth compared to the distance to these infinitely far away stars is, within the accuracy of the measurement, 0. Thus a line of sight from Earth's first position E to vertex v will be essentially the same as a line of sight from the Earth's second position E' to the same vertex v, and will therefore run parallel to it - impossible to depict convincingly in an image of limited size:

Since line E'-v' is a transversal in the same (approximately Euclidian) plane as parallel lines E-v and E'-v, it follows that the corresponding angles of intersection of these parallel lines with this transversal are congruent: the angle θ between lines of sight E-v and E'-v' is equal to the angle θ between E'-v and E'-v', which is the angle θ between observed positions of S in relation to its apparently unmoving stellar surroundings.

The distance *d* from the Sun to S now follows from simple trigonometry:

tan(½θ) = E-Sun / d,

so that d = E-Sun / tan(½θ), where E-Sun is 1 AU.

The more distant an object is, the smaller its parallax.

Stellar parallax measures are given in the tiny units of arcseconds, or even in thousandths of arcseconds (milliarcseconds). The distance unit parsec is defined as the length of the leg of a right triangle adjacent to the angle of one arcsecond at one vertex, where the other leg is 1 AU long. Because stellar parallaxes and distances all involve such skinny right triangles, a convenient trigonometric approximation can be used to convert parallaxes (in arcseconds) to distance (in parsecs). The approximate distance is simply the reciprocal of the parallax: For example, Proxima Centauri (the nearest star to Earth other than the Sun), whose parallax is 0.7685, is 1 / 0.7685 parsecs = 1.301 parsecs (4.24 ly) distant.^{[1]}

## Early theory and attempts

Stellar parallax is so small that it was unobservable until the 19th century, and its apparent absence was used as a scientific argument against heliocentrism during the early modern age. It is clear from Euclid's geometry that the effect would be undetectable if the stars were far enough away, but for various reasons, such gigantic distances involved seemed entirely implausible: it was one of Tycho Brahe's principal objections to Copernican heliocentrism that for it to be compatible with the lack of observable stellar parallax, there would have to be an enormous and unlikely void between the orbit of Saturn and the eighth sphere (the fixed stars).^{[2]}

James Bradley first tried to measure stellar parallaxes in 1729. The stellar movement proved too insignificant for his telescope, but he instead discovered the aberration of light^{[3]} and the nutation of Earth's axis, and catalogued 3222 stars.

## 19th and 20th centuries

Stellar parallax is most often measured using *annual parallax*, defined as the difference in position of a star as seen from Earth and Sun, i.e. the angle subtended at a star by the mean radius of Earth's orbit around the Sun. The parsec (3.26 light-years) is defined as the distance for which the annual parallax is 1 arcsecond. Annual parallax is normally measured by observing the position of a star at different times of the year as Earth moves through its orbit. Measurement of annual parallax was the first reliable way to determine the distances to the closest stars. The first successful measurements of stellar parallax were made by Friedrich Bessel in 1838 for the star 61 Cygni using a heliometer.^{[4]}^{[5]}

Being very difficult to measure, only about 60 stellar parallaxes had been obtained by the end of the 19th century, mostly by use of the filar micrometer. Astrographs using astronomical photographic plates sped the process in the early 20th century. Automated plate-measuring machines^{[6]} and more sophisticated computer technology of the 1960s allowed more efficient compilation of star catalogues. In the 1980s, charge-coupled devices (CCDs) replaced photographic plates and reduced optical uncertainties to one milliarcsecond.^{[citation needed]}

Stellar parallax remains the standard for calibrating other measurement methods (see Cosmic distance ladder). Accurate calculations of distance based on stellar parallax require a measurement of the distance from Earth to the Sun, now known to exquisite accuracy based on radar reflection off the surfaces of planets.^{[7]}

The angles involved in these calculations are very small and thus difficult to measure. The nearest star to the Sun (and also the star with the largest parallax), Proxima Centauri, has a parallax of 0.7685 ± 0.0002 arcsec.^{[1]} This angle is approximately that subtended by an object 2 centimeters in diameter located 5.3 kilometers away.

A large heliometer was installed at Kuffner Observatory (In Vienna) in 1896, and was used for measuring the distance to other stars by trigonometric parallax.^{[8]} By 1910 it had computed 16 parallax distances to other stars, out of only 108 total known to science at that time.^{[8]}

## Space astrometry for parallax

In 1989 the satellite Hipparcos was launched primarily for obtaining parallaxes and proper motions of nearby stars, increasing the number of stellar parallaxes measured to milliarcsecond accuracy a thousandfold. Even so, Hipparcos is only able to measure parallax angles for stars up to about 1,600 light-years away, a little more than one percent of the diameter of the Milky Way Galaxy.

The Hubble telescope WFC3 now has a precision of 20 to 40 microarcseconds, enabling reliable distance measurements up to 3,066 parsecs (10,000 ly) for a small number of stars.^{[10]} This gives more accuracy to the Cosmic distance ladder and improves the knowledge of distances in the Universe, based on the dimensions of the Earth's orbit.

The European Space Agency's Gaia mission, launched 19 December 2013, is expected to measure parallax angles to an accuracy of 10 microarcseconds for all moderately bright stars, thus mapping nearby stars (and potentially planets) up to a distance of tens of thousands of light-years from Earth.^{[11]} Data Release 2 in 2018 claims mean errors for the parallaxes of 15th magnitude and brighter stars of 20–40 microarcseconds.^{[12]}

### Radio astrometry for parallax

Very long baseline interferometry in the radio band can produce images with angular resolutions of about 1 milliarcsecond, and hence, for bright radio sources, the precision of parallax measurements made in the radio can easily exceed those of optical telescopes like Gaia. These measurements tend to be sensitivity limited, and need to be made one at a time, so the work is generally done only for sources like pulsars and X-ray binaries, where the radio emission is strong relative to the optical emission.^{[citation needed]}

## Other baselines

### Statistical parallax

Two related techniques can determine the mean distances of stars by modelling the motions of stars. Both are referred to as statistical parallaxes, or individual called secular parallaxes and classical statistical parallaxes.

The motion of the Sun through space provides a longer baseline that will increase the accuracy of parallax measurements, known as secular parallax. For stars in the Milky Way disk, this corresponds to a mean baseline of 4 AU per year, whereas for halo stars the baseline is 40 AU per year. After several decades, the baseline can be orders of magnitude greater than the Earth–Sun baseline used for traditional parallax. However, secular parallax introduces a higher level of uncertainty because the relative velocity of other stars is an additional unknown. When applied to samples of multiple stars, the uncertainty can be reduced; the precision is inversely proportional to the square root of the sample size.^{[13]}

The mean parallaxes and distances of a large group of stars can be estimated from their radial velocities and proper motions. This is known as a classical statistical parallax. The motions of the stars are modelled to statistically reproduce the velocity dispersion based on their distance.^{[13]}^{[14]}

## Other parallax in astronomy

Other uses of the term parallax in astronomy, none of which actually utilise a parallax, are the photometric parallax method, spectroscopic parallax, and dynamical parallax.

## See also

- Apparent place
- TAU (spacecraft) (an abandoned space mission project that would have used parallax)

## References

- ^
^{a}^{b}Brown, A. G. A.; et al. (Gaia collaboration) (August 2018). "*Gaia*Data Release 2: Summary of the contents and survey properties".*Astronomy & Astrophysics*.**616**. A1. arXiv:1804.09365. Bibcode:2018A&A...616A...1G. doi:10.1051/0004-6361/201833051. **^**See p.51 in*The reception of Copernicus' heliocentric theory: proceedings of a symposium organized by the Nicolas Copernicus Committee of the International Union of the History and Philosophy of Science*, Torun, Poland, 1973, ed. Jerzy Dobrzycki, International Union of the History and Philosophy of Science. Nicolas Copernicus Committee; ISBN 90-277-0311-6, ISBN 978-90-277-0311-8**^**Buchheim, Robert (4 October 2007).*The Sky is Your Laboratory*. ISBN 978-0-387-73995-3. Page 184.**^**Zeilik & Gregory 1998, p. 44.**^**Bessel, FW, "Bestimmung der Entfernung des 61sten Sterns des Schwans Archived 2007-06-24 at the Wayback Machine" (1838)*Astronomische Nachrichten*, vol. 16, pp. 65–96.**^**CERN paper on plate measuring machine USNO StarScan**^**Zeilik & Gregory 1998, § 22-3.- ^
^{a}^{b}Habison, Peter (1998). "Astrometry and early astrophysics at Kuffner Observatory in the late 19th century".*Acta Historica Astronomiae*.**3**: 93–94. Bibcode:1998AcHA....3...93H. ISSN 0003-2670. **^**"Hubble stretches the stellar tape measure ten times further".*ESA/Hubble Images*. Retrieved 12 April 2014.**^**Harrington, J.D.; Villard, Ray (10 April 2014). "NASA's Hubble Extends Stellar Tape Measure 10 Times Farther into Space".*NASA*. Retrieved 17 October 2014.Riess, Adam G.; Casertano, Stefano; Anderson, Jay; Mackenty, John; Filippenko, Alexei V. (2014). "Parallax Beyond a Kiloparsec from Spatially Scanning the Wide Field Camera 3 on the Hubble Space Telescope".*The Astrophysical Journal*.**785**(2): 161. arXiv:1401.0484. Bibcode:2014ApJ...785..161R. doi:10.1088/0004-637X/785/2/161.**^**Henney, Paul J. "ESA's Gaia Mission to study stars". Astronomy Today. Retrieved 8 March 2008.**^**Brown, A. G. A.; et al. (Gaia collaboration) (August 2018). "*Gaia*Data Release 2: Summary of the contents and survey properties".*Astronomy & Astrophysics*.**616**. A1. arXiv:1804.09365. Bibcode:2018A&A...616A...1G. doi:10.1051/0004-6361/201833051.- ^
^{a}^{b}Popowski, Piotr; Gould, Andrew (29 January 1998). "Mathematics of Statistical Parallax and the Local Distance Scale". arXiv:astro-ph/9703140. Bibcode:1997astro.ph..3140P. Cite journal requires`|journal=`

(help) **^**Layden, Andrew C; Hanson, Robert B; Hawley, Suzanne L; Klemola, Arnold R; Hanley, Christopher J (1996). "The Absolute Magnitude and Kinematics of RR Lyrae Stars Via Statistical Parallax".*The Astronomical Journal*.**112**: 2110. arXiv:astro-ph/9608108. Bibcode:1996AJ....112.2110L. doi:10.1086/118167.

- Hirshfeld, Alan w. (2001).
*Parallax: The Race to Measure the Cosmos*. New York: W. H. Freeman. ISBN 0-7167-3711-6.CS1 maint: ref=harv (link) - Whipple, Fred L. (2007).
*Earth Moon and Planets*. Read Books. ISBN 978-1-4067-6413-0.CS1 maint: ref=harv (link). - Zeilik, Michael A.; Gregory, Stephan A. (1998).
*Introductory Astronomy & Astrophysics*(4th ed.). Saunders College Publishing. ISBN 0-03-006228-4.CS1 maint: ref=harv (link).

## Further reading

- Dyson, F. W. (1915). "Measurement of the distances of the stars".
*The Observatory*.**38**: 292. Bibcode:1915Obs....38..292D.