|
|
|
|
Proper motion
|
| |
|
| |
The proper motion of a star is its angular change in position over time as seen from the Sun, as inferred after improper motions are accounted for. It is measured in seconds of arc per year, arcsec/yr (3600 arcsec = 1 degree). This contrasts with radial velocity, which is the time rate of change in distance toward or away from the viewer, usually measured by Doppler shift of received radiation. The proper motion is not entirely "proper" (that is, intrinsic to the star) because it includes a component due to the motion of the Sun itself.
Introduction
Over the course of centuries, stars appear to maintain nearly fixed positions with respect to each other, so that they form the same constellations over historical time.
Discussion
Ask a question about 'Proper motion' Start a new discussion about 'Proper motion' Answer questions from other users |
Encyclopedia
The proper motion of a star is its angular change in position over time as seen from the Sun, as inferred after improper motions are accounted for. It is measured in seconds of arc per year, arcsec/yr (3600 arcsec = 1 degree). This contrasts with radial velocity, which is the time rate of change in distance toward or away from the viewer, usually measured by Doppler shift of received radiation. The proper motion is not entirely "proper" (that is, intrinsic to the star) because it includes a component due to the motion of the Sun itself.
Introduction
Over the course of centuries, stars appear to maintain nearly fixed positions with respect to each other, so that they form the same constellations over historical time. Ursa Major, for example, looks nearly the same now as it did hundreds of years ago. However, precise long-term observations show that the constellations change shape, albeit very slowly, and that each star has an independent motion.
This motion is caused by the true movement of the stars relative to the Sun and solar system through space. The Sun travels in a nearly circular orbit (the solar circle) about the center of the Milky Way at a speed of about 220 km/s at a radius of 8 ± 0.65 kpc from the center, which can be taken as the rate of rotation of the Milky Way itself at this radius.
The proper motion is measured by two quantities: the position angle and the proper motion itself. The first quantity indicates the direction of the proper motion on the celestial sphere (with 0 degrees meaning the motion due north, 90 degrees due east, and so on), and the second quantity gives the motion's magnitude, in seconds of arc per year.
. The celestial north pole is CNP, the vernal equinox is V, the star path on the celestial sphere is indicated by arrows. The proper motion vector is µ, a = right ascension, d = declination, ? = position angle. ]]
Proper motion may also be given by the angular changes per year in the right ascension (µa) and declination (µd). On the celestial sphere, positions are located by latitude and longitude. The coordinate d corresponds to latitude. The coordinate a corresponds to longitude measured from the vernal equinox V, the point on the sky where the Sun crosses the celestial equator on near March 21.
The components of proper motion by convention are arrived at as follows. Suppose in a year an object moves from coordinates (a, d) to coordinates (a1, d1), with angles measured in seconds of arc. Then the changes of angle in seconds of arc per year are:
The magnitude of the proper motion µ is given by vector addition of its components:
where d is the declination. The factor in cos d accounts for the fact that the radius from the axis of the sphere to its surface varies as cos d, becoming, for example, zero at the pole. Thus, the component of velocity parallel to the equator corresponding to a given angular change in a is smaller the further north the object's location. The change µa , which must be multiplied by cos d to become a component of the proper motion, is sometimes called the "proper motion in right ascension", and µd the "proper motion in declination".
The position angle ? is related to these components by:
Barnard's star has the largest proper motion of all stars, moving at 10.3 seconds of arc per year. Large proper motion is usually a strong indication that a star is relatively close to the Sun. This is indeed the case for Barnard's Star which, at a distance of about 6 light-years, is, after the Sun and the Alpha Centauri system, the nearest known star to Earth (yet, being a red dwarf, too faint to see without a telescope or powerful binoculars, with an apparent magnitude of 9.54).
In 1992, Rho Aquilae became the first star to have its name invalidated by moving to a neighbouring constellation - it is now a star of the
constellation Delphinus. This will next happen to Gamma Caeli,
which is due to become a star of the constellation Columba in the year 2400.
A proper motion of 1 arcsec per year at a distance of 1 light-year corresponds to a relative transverse speed of 1.45 km/s. For Barnard's star this works out to 90 km/s; including the radial velocity of 111 km/s (which is at right angles to the transverse velocity) gives a true motion of 142 km/s. True or absolute motion is more difficult to measure than the proper motion, as the true transverse velocity involves the product of the proper motion times the distance; that is, true velocity measurements depend on distance measurements, which are difficult in general. Currently, the nearby star with the largest true velocity (relative to the Sun) is Wolf 424 which moves at 555 km/s (or 1/540 of the speed of light).
Usefulness in Astronomy
Stars with large proper motions tend to be nearby; most stars are far enough away that their proper motions are very small, of order a few thousandths of an arcsecond per year. It is possible to construct nearly complete samples of high proper motion stars by comparing photographic sky survey images taken many years apart. The Palomar Sky Survey is one source of such images. In the past, searches for high proper motion objects were undertaken using blink comparators to examine the images by eye, but modern efforts use techniques such as image differencing to automatically search through digitized image data. Because the selection biases of the resulting high proper motion samples are well-understood and well-quantified, it is possible to use them to construct an unbiased census of the nearby stellar population — how many stars exist of each true brightness, for example. Studies of this kind show that the local population of stars consists largely of intrinsically faint, inconspicuous stars such as red dwarfs.
Measurement of the proper motions of a large sample of stars in a distant stellar system, like a globular cluster, can be used to compute the cluster's total mass via the Leonard-Merritt mass estimator. Coupled with measurements of the stars' radial velocities, proper motions can be used to compute the distance to the cluster.
NGC 4258 located about 25 million light years away (7.2 ± 0.5 Mpc) in the constellation Canes Venatici. From ]]
Stellar proper motions have been used to infer the presence of a super-massive black hole at the center of the Milky Way. This black hole is suspected to be Sgr A*, with a mass of 2.6 × 106 M?, where M? is a solar mass.
Proper motions of the galaxies in the Local Group are discussed in detail in Röser. In 2005, the first measurement was made of the proper motion of the Triangulum Galaxy M-33, the third largest and only ordinary spiral galaxy in the Local Group, located 860 ± 28 kpcs beyond the Milky Way. Although the Andromeda galaxy is known to move, and an Andromeda-Milky Way collision is predicted in about 5 – 10 billion years, the proper motion of the Andromeda galaxy, about 786 kpc distant, is still an uncertain matter, with an upper bound on its transverse velocity of ˜ 100 km/s. Proper motion of the NGC 4258 (M106) galaxy in the M106 group of galaxies was used in 1999 to find an accurate distance to this object. Measurements were made of the radial motion of objects in that galaxy moving directly toward and away from us, and assuming this same motion to apply to objects with only a proper motion, the observed proper motion predicts a distance to the galaxy of 7.2 ± 0.5 Mpc.
History
Proper motion was suspected by early astronomers (according to Macrobius, AD 400) but proof was provided in 1718 by Edmund Halley, who noticed that Sirius, Arcturus and Aldebaran were over half a degree away from the positions charted by the ancient Greek astronomer Hipparchus roughly 1850 years earlier.
Stars with high proper motion
The following are the stars with highest proper motion from the Hipparcos catalog. It does not include stars such as Teegarden's star which are too faint for that catalog.
Highest proper motion stars | # | Star | Proper motion | Radial
velocity
(km/s) | Parallax
(mas) |
|---|
µa
(mas/yr) | µd
(mas/yr) |
|---|
| 1 | Barnard's star | -798.71 | 10337.77 | -106.8 | 549.30 | | 2 | Kapteyn's star | 6500.34 | -5723.17 | +245.5 | 255.12 | | 3 | Groombridge 1830 | 4003.69 | -5814.64 | -98.0 | 109.22 | | 4 | Lacaille 9352 | 6766.63 | 1327.99 | +9.7 | 303.89 | | 5 | CD -37 15492 (GJ 1) | 5633.95 | -2336.69 | +23.6 | 229.32 | | 6 | HIP 67593 | 5369.33 | — | 76.20 | | 7 | 61 Cygni A & B | 4133.05 | 3201.78 | -64.3 | 287.18 | | 8 | Lalande 21185 | -580.46 | -4769.95 | -85.0 | 392.52 | | 9 | Epsilon Indi | 3961.41 | -2538.33 | -40.4 | 275.79 |
Software
There are a number software products that allow a person to view the proper motion of stars over differing time scales. Two free ones are:
- - Freeware - Windows, Fairly Basic. You can choose a region of the sky, set the limiting magnitude and set a time sequence (time step, number of steps, and step interval). The program will simulate the motion of the stars. There's a clear help function included.
- - Freeware - Windows, Moderately sophisticated, with some pretty displays. Still under development, needs some more navigation and configuration features.
See also
External links
|
| |
|
|
