n.
A star whose brightness varies because of internal changes or periodic eclipsing of mutually revolving stars.
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A star whose brightness varies because of internal changes or periodic eclipsing of mutually revolving stars.
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A star that has a detectable change in brightness which is often accompanied by other physical changes. During the life of a star, changes in brightness occur in the early stages, while it is forming, or in the late stages, close to its death. Therefore, variability provides important clues about the evolution and nature of stars. Depending upon the type of star, variability in brightness can provide information about its size, radius, mass, temperature, luminosity, internal and external structure, composition, and distance from the Earth. Over 31,900 stars are known to vary in brightness.
Variable stars can be divided into two major types: extrinsic and intrinsic variables. The extrinsic variables are those stars in which the variability in brightness occurs because of the occultation of one star by another (eclipsing binary) or rotation of a star that has dark or bright spots on its surface, similar to sunspots. See also Binary star; Eclipsing variable stars.
Intrinsic variables are those stars in which the variability of brightness occurs because of physical change in or on the star itself. These stars are divided into two classes: pulsating and eruptive.
Pulsating variables
Periodic pulsation (contraction and expansion) of the star and its outer layer results in the variation in brightness, as well as variations in the star's temperature, spectrum, and radius.
Cepheids are rare, highly luminous (supergiant), yellow variable stars. They vary with periods from 1 to 100 days, and have a range of variation from 0.1 to 2 magnitudes. Cepheids show an important correlation between their period of variation and their relative brightness, in that those stars with longer periods are also brighter. Due to this period-luminosity relationship, cepheids have been used to measure distances to nearby galaxies and in the determination of the distance scale of the universe.
A similar group of variable stars, W Virginis stars, found in globular star clusters and the corona of the Milky Way Galaxy, are bluer (and thus hotter) and older (population II) than the cepheids. They have periods from 10 to 30 days, and obey a similar period-luminosity relationship. They are sometimes called type II cepheids to distinguish them from the classical type I cepheids. See also Cepheids.
RR Lyrae variables are the second most common type of variable in the Galaxy. They have periods of less than 1 day, and have a small range of variation, from 0.5 to 1.5 magnitudes. They are particularly numerous in globular clusters, and thus are sometimes referred to as cluster variables. All RR Lyrae variables have the same intrinsic luminosity, of magnitude 0.5. Thus, if an RR Lyrae star can be identified in a star cluster and its apparent magnitude determined, the above equation and the star's known absolute magnitude can be used to obtain the distance to the cluster.
Long-period variable stars are the most abundant of all variables in the Milky Way Galaxy. They are red, cool, giant or supergiant stars with spectral class M or R, S, or C carbon types. Long-period variables are old stars which have evolved from the main sequence and are in the late stages of their evolution. See also
The prototype of long-period variables is o Ceti (Mira), which has given its name to those long-period variables that have a range of variation of 2.5 magnitudes and more. Mira variables have periods ranging from 100 to 1000 days. Although the change in brightness is periodic, some cycles may be much brighter or fainter than others. See also Mira.
Red giant and supergiant stars with less regularity of variation, shorter periods, and smaller ranges of variation, less than 2.5 magnitudes, are called semiregular variables. Other red variable stars that do not exhibit any regularity in their brightness change are called irregular stars.
Rare, very luminous, yellow supergiant stars that generally show alternating shallow and deep fadings are called RV Tauri stars. These pulsating variables vary by 2 to 3 magnitudes within 30 to 150 days.
Eruptive variables
Eruptive variables are those stars that have one or more eruptions—the ejection of matter into space—in their lifetime. The most spectacular type of stellar explosion is that of a supernova, wherein a star's luminosity suddenly increases to tens of thousands of times the original brightness and the star outshines the total brightness of its galaxy. The gigantic explosion may be due to the gravitational collapse of a very hot and massive star that has exhausted the energy available from nuclear reactions; the collapse then creates enormous energy to blast outward the layers surrounding the stellar core. Alternatively, the explosion may occur in a close binary system in which one of the components is a massive white dwarf, an Earth-sized, very compact, old star, that explodes when it receives too much material from the other component. See also Supernova.
Cataclysmic variables are very close binary systems made up of an evolved, hot, dense white dwarf and a less evolved cool star which transfers mass onto the white dwarf accretion disk. The best known of the cataclysmic variables are stars that brighten by 7 to 16 magnitudes within about a day. They stay at maximum brightness for a few days or weeks and then slowly fade. The word nova, meaning new, was used for these stars. Actually a nova is not a new star, but an already existing star which due to the eruption has become very luminous and thus visible. Recurrent novae are stars that about evey 20 years or more have eruptions during which the system brightens by 7 to 9 magnitudes. Dwarf novae have smaller-scale eruptions, in which the star brightens by 2 to 6 magnitudes within a day, stays bright 1 to 2 weeks, and then fades to the original brightness.
R Coronae Borealis stars, instead of brightening through eruptions, irregularly decrease in brightness every 2 to 3 years by 1 to 9 magnitudes. The decrease in brightness is caused by the veiling of the star by thick carbon clouds expelled to the star's atmosphere. See also Cataclysmic variable; Star.
Nebular variables are young stars in the early stages of stellar formation.
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Intrinsic Variable Stars
Pulsating Variables
Pulsating variables account for more than half of the known variable stars. They are characterized by slight instabilities that cause the star alternately to expand and contract. This pulsation is accompanied by changes in absolute luminosity and temperature. The pulsating variables can be further divided into the following subclasses: short-term, long-term, semiregular, and irregular. Short-term variables have well-defined periods ranging from less than one day to more than 50 days.
Relatively rare among this subclass are the Cepheid variables; these yellow supergiant stars are historically important because, having periods roughly proportional to their absolute brightness, they provide a means of measuring galactic and extragalactic distances. A key research program of the Hubble Space Telescope is the measurement of Cepheid variables in distant galaxies in order to refine our concept of the size and age of the universe. Cepheid variables are classed as either population I Cepheids, which are found in the spiral arms of galaxies, or population II Cepheids, also known as W Virginis stars, which are found in star clusters (see also stellar populations). About 700 Cepheids of both types have been found in our galaxy.
A more common short-term variable is of the RR Lyrae group; about 6,000 of this type are known in our galaxy and are concentrated in globular clusters. They have periods of less than one day, and all have roughly the same intrinsic brightness. The latter feature, along with their wide distribution throughout the galaxy, makes them another useful distance indicator.
The long-term variables are the most numerous of all pulsating stars. They are red giant and supergiant stars with periods ranging from a few months to more than a year. The best known of these stars is Omicron Ceti, also known as Mira. Over a period of about 11 months, it brightens by about 7 magnitudes and then gradually fades. Semiregular variables are stars whose periodic variations are occasionally interrupted by sudden bursts of light. The best-known example is the red supergiant Betelgeuse, in Orion. Irregular variables show no periodicity in their variations in brightness. The amplitude of their fluctuations in brightness is in general smaller than the fluctuations of the long-term regular variables.
Eruptive Variables
The eruptive variables are highly unstable stars that suddenly and unpredictably increase in brightness. T Tauri stars, also known as nebular variables because they are young objects still embedded in nebulosity, are the least violent of these explosive stars. Novas and supernovas are much more dramatic. Novas are small, very hot stars that suddenly increase thousands of times in luminosity. Their decline in luminosity is much slower, taking months or even years. Most novas probably repeat their outbursts, the dwarf novas every few months, the recurring novas every few years or decades, and the standard novas over thousands of years. Supernovas, upon exploding, increase millions of times in brightness and are totally disrupted. More than 30 supernovas events are observed annually in distant galaxies. Three supernovas have been seen in our own galaxy, in 1054, 1572, and 1604; in 1987 a supernova erupted in a neighboring galaxy, the Large Magellanic Cloud.
Extrinsic Variable Stars
Eclipsing variables are not true (intrinsic) variables but rather are binary star systems, i.e., pairs of stars revolving around a common center of mass. The apparent brightness of an eclipsing variable fluctuates because the orbit of the pair is seen edgewise, so that first one star and then the other regularly blocks the light of its companion. Best known of this type is Algol (Beta Persei).
Bibliography
See D. Levy, Observing Variable Stars (1989).
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A star is classified as variable if its apparent brightness as seen from Earth changes over time, whether the changes are due to variations in the star's actual luminosity, or to variations in the amount of the star's light that is blocked from reaching Earth. Many, possibly most, stars have at least some variation in luminosity: the energy output of our Sun, for example, varies by about 0.1% over an 11 year solar cycle,[1] equivalent to a change of one thousandth of a magnitude. Astronomers use the term millimagnitude, abbreviated as mmag, for one thousandth of a magnitude.
It is convenient to classify variable stars as belonging to one of two types:
The first variable star was identified in 1638 when Johannes Holwarda noticed that Omicron Ceti (later named Mira) pulsated in a cycle taking 11 months; the star had previously been described as a nova by David Fabricius in 1596. This discovery, combined with supernovae observed in 1572 and 1604, proved that the starry sky was not eternally invariable as Aristotle and other ancient philosophers had taught. In this way, the discovery of variable stars contributed to the astronomical revolution of the sixteenth and early seventeenth centuries.
The second to be described variable star was the eclipsing variable Algol by Geminiano Montanari in 1669; John Goodricke in 1784 gave the correct explanation of its variability. In order of discovery Chi Cygni was next, 1686 by G. Kirch, then R Hydrae in 1704 by G. D. Maraldi, and so on. By 1786 ten variable stars were known. John Goodricke himself discovered Delta Cephei and Beta Lyrae. Since 1850 the number of known variable stars has increased rapidly, especially after 1890 when it became possible to identify variable stars by means of photography.
The latest edition of the General Catalogue of Variable Stars[2] (2008) lists more than 46,000 variable stars in our own galaxy, as well as 10,000 in other galaxies, and over 10,000 'suspected' variables.
The most common kinds of variability involve changes in brightness, but other types of variability also occur, in particular changes in the spectrum. By combining light curve data with observed spectral changes, astronomers are often able to explain why a particular star is variable.
Variable stars are generally analysed using photometry, spectrophotometry and spectroscopy. Measurements of their changes in brightness can be plotted to produce light curves. For regular variables, the period of variation and its amplitude can be very well established; for many variable stars, though, these quantities may vary slowly over time, or even from one period to the next. Peak brightnesses in the light curve are known as maxima, while troughs are known as minima.
Amateur astronomers can do useful scientific study of variable stars by visually comparing the star with other stars within the same telescopic field of view of which the magnitudes are known and constant. By estimating the variable's magnitude and noting the time of observation a visual lightcurve can be constructed. The American Association of Variable Star Observers collects such observations from participants around the world and shares the data with the scientific community.
From the light curve the following data are derived:
From the spectrum the following data are derived:
In very few cases it is possible to make pictures of a stellar disk. These may show darker spots on its surface.
Combining light curves with spectral data often gives a clue as to the changes that occur in a variable star. For example, a pulsating star betrays itself in its spectrum because its surface periodically moves to and from us, in the same tempo as its brightness varies.
About two-thirds of all variable stars appear to be pulsating. In the 1930s astronomer Arthur Stanley Eddington showed that the mathematical equations that describe the interior of a star may lead to instabilities that cause a star to pulsate. The most common type of instability is related to oscillations in the degree of ionization in outer, convective layers of the star.
Suppose the star is in the swelling phase. Its outer layers expand, causing them to cool. Because of the decreasing temperature the degree of ionization also decreases. This makes the gas more transparent, and thus makes it easier for the star to radiate its energy. This in turn will make the star start to contract. As the gas is thereby compressed, it is heated and the degree of ionization again increases. This makes the gas more opaque, and radiation temporarily becomes captured in the gas. This heats the gas further, leading it to expand once again. Thus a cycle of expansion and compression (swelling and shrinking) is maintained.
The pulsation of cepheids is known to be driven by oscillations in the ionization of helium (from He++ to He+ and back to He++).
In a given constellation, the first variable stars discovered were designated with letters R through Z, e.g. R Andromedae. This system of nomenclature was developed by Friedrich W. Argelander, who gave the first previously unnamed variable in a constellation the letter R, the first letter not used by Bayer. Letters RR through RZ, SS through SZ, up to ZZ are used for the next discoveries, e.g. RR Lyrae. Later discoveries used letters AA through AZ, BB through BZ, and up to QQ through QZ (with J omitted). Once those 334 combinations are exhausted, variables are numbered in order of discovery, starting with the prefixed V335 onwards.
Variable stars may be either intrinsic or extrinsic.
These subgroups themselves are further divided into specific types of variable stars that are usually named after their prototype. For example, dwarf novae are designated U Geminorum stars after the first recognized star in the class, U Geminorum.
Examples of types within these divisions are given below.
The pulsating stars[3] swell and shrink regularly by stellar radius, magnitude and spectrum, most often with a defined period, sometimes semiregularly with an average period and amplitude, or a pseudoperiod. The two most important types are:
This group consists of several kinds of pulsating stars that swell and shrink very regularly by the star's own mass resonance, generally by the fundamental frequency. Generally the Eddington valve mechanism for pulsating variables is believed to account for cepheid like pulsations: a certain helium layer of the star has variable opacity depending on the ionization degree, greater opacity for the greater level of ionization. At minimum the star is contracted so that the layer has the higher ionization and opacity, and therefore absorbs fusion energy for the star to expand. When the star swells up to a certain size, the ionization suddenly switches from higher to lower, switching the opacity to lower too. The inner fusion energy now radiates easier through this star layer, so the star shrinks to the original contracted state, and the cycle begins anew.
Delta Cepheid, W Virginids, RR Lyrae variables and Delta Scutids belong to the instability strip which is believed to be driven by Eddington pulsations in helium, while for the Beta Cepheids the pulsation mechanism is unknown. The instability strip stars are spectral type late A through M stars (from "white" to "red" by convention). Beta cepheids belongs to type B or sometimes late O ("blue" and deeper "blue").
Generally in each subgroup a fixed relation holds between period and absolute magnitude, as well as a relation between period and mean density of the star. This period-luminosity relationship was first established for Delta Cepheids by Henrietta Swan Leavitt.
One of the most important types of variables star are Delta Cephei variables, yellow giant stars which undergo pulsations with very regular periods. Usually referred to simply as Cepheid variables, they are named after Delta Cephei (δ Cep), the first of the class to be discovered, and have periods ranging from about a day to several weeks.
Cepheids are important because they are a type of standard candle. Their luminosity is directly related to their period of variation, with a slight dependence on metallicity as well. The longer the pulsation period, the more luminous the star. Once this period-luminosity relationship is calibrated, the luminosity of a given Cepheid whose period is known can be established. Their distance is then easily found from their apparent brightness. Observations of Cepheid variables are very important for determining distances to galaxies within the Local Group and beyond.
Edwin Hubble used this method to prove that the so-called spiral nebulae are in fact distant galaxies.
Of the brighter stars in the sky, Polaris is a Cepheid, although a somewhat unusual one.
W Virginis stars have clock regular light pulsations and a luminosity relation much like the δ Cephei variables, so initially they were confused with the latter category. Comparing the light curve, the amplitude and the radial velocity variations as compared to the light curve, W Virginis constitute a different class of star with a luminosity relation offset from that of the δ Cepheids. W Virginis stars also belong to Population II, compared to Population I of δ Cepheids, and so have a lower metallicity.
These stars are somewhat similar to Cepheids, but are not as luminous. They are older than cepheids, belonging to Population II. Due to their common occurrence in globular clusters, they are occasionally referred to as cluster Cepheids. They also have a well established period-luminosity relationship, and so are also useful distance indicators. These spectral type A stars vary by about 0.2 - 2 magnitudes (20% to over 500% change in luminosity) over a period of several hours to a day or more. Their brightness is greatest when their radii are at their maximum.
Delta Scuti (δ Sct) variables are similar to Cepheids but rather fainter, and with shorter periods. They were once known as Dwarf Cepheids. They often show many superimposed periods, which combine to form an extremely complex light curve. The typical δ Scuti star has an amplitude of 0.003 - 0.9 magnitudes (0.3% to about 130% change in luminosity) and a period of 0.01 - 0.2 days. Their spectral type is usually between A0 and F5.
These stars of spectral type A2 to F5, similar to δ Scuti variables, are found mainly in globular clusters. They exhibit fluctuations in their brightness in the order of 0.7 magnitude (about 100% change in luminosity) or so every 1 to 2 hours.
Bluewhite stars, often giants, with small brightness variations and short periods.
Beta Cephei (β Cep) variables, or Beta Canis Majoris variables, as these stars are sometimes called, especially in Europe)[4] undergo short period pulsations in the order of 0.1 - 0.6 days with an amplitude of 0.01 - 0.3 magnitudes (1% to 30% change in luminosity). They are at their brightest during minimum contraction. Many stars of this kind exhibits multiple pulsation periods.
Stars in this class are type Bp supergiants with a period of 0.1 - 1 day and an amplitude of 0.1 magnitude on average. Their spectra are peculiar by having weak hydrogen while on the other hand carbon and helium lines are extra strong.
Various groups of red giant stars that pulsate with periods in the range of weeks to several years. The period is not always constant but changes from cycle to cycle.
Mira variables are very cool red supergiants, which are undergoing very large pulsations. The mechanism is believed to be Eddington pulsations, like for the yellow Cepheids (see above), but with molecular hydrogen as the variable opacity layer of the star instead of helium. Since hydrogen is the most abundant element almost everywhere in Universe and in stars, the pulsations generally have a great amplitude. Over periods of usually many months, they may brighten by between 2.5 and up to 11 magnitudes (six-fold to 30 thousand-fold change in luminosity) before fading again. Mira itself, also known as Omicron Ceti (ο Cet), varies in brightness from almost 2nd magnitude to as faint as 10th magnitude with a period of roughly 332 days.
These are usually red giants or supergiants. Semiregular variables may show a definite period on occasion, but also go through periods of irregular variation. A well-known example of a semiregular variable is Betelgeuse, which varies from about magnitudes +0.2 to +1.2 (20% to 200% change in luminosity).
These are usually red supergiants with little or no periodicity. They are often poorly studied semiregular variables that, upon closer scrutiny, should be reclassified.
These are yellow supergiant stars which have alternating deep and shallow minima. This double-peaked variation typically has periods of 30-100 days and amplitudes of 3 - 4 magnitudes. Superimposed on this variation, there may be long-term variations over periods of several years. Their spectra are of type F or G at maximum light and type K or M at minimum brightness.
Alpha Cygni (α Cyg) variables are nonradially pulsating supergiants of spectral classes Bep to AepIa. Their periods range from several days to several weeks, and their amplitudes of variation are typically of the order of 0.1 magnitudes (10% change in luminosity). The light changes, which often seem irregular, are caused by the superposition of many oscillations with close periods. Deneb, in the constellation of Cygnus is the prototype of this class.
These non-radially pulsating stars have short periods of hundreds to thousands of seconds with tiny fluctuations of 0.001 to 0.2 magnitudes. Known types of pulsating white dwarf (or pre-white dwarf) include the DAV, or ZZ Ceti, stars, with hydrogen-dominated atmospheres and the spectral type DA;[5] DBV, or V777 Her, stars, with helium-dominated atmospheres and the spectral type DB;[6] and GW Vir stars, with atmospheres dominated by helium, carbon, and oxygen. GW Vir stars may be subdivided into DOV and PNNV stars.[7][8]
The Sun oscillates with very low amplitude in a large number of modes having periods around 5 minutes. The study of these oscillations is known as helioseismology. Oscillations in the Sun are driven stochastically by convection in its outer layers. The term solar-like oscillations is used to describe oscillations in other stars that are excited in the same way and the study of these oscillations is known as asteroseismology.
Protostars are young objects that have not yet completed the process of contraction from a gas nebula to a veritable star. Most protostars exhibit irregular brightness variations.
Variability of more massive (2-8 solar mass) Herbig Ae/Be stars is thought to be due to gas-dust clumps, orbiting in the circumstellar disks.
Orion variables are young, hot pre-main sequence stars usually embedded in nebulosity. They have irregular periods with amplitudes of several magnitudes. A well known subtype of Orion variables are the T Tauri variables. Variability of T Tauri stars is due to spots on the stellar surface and gas-dust clumps, orbiting in the circumstellar disks.
These stars reside in reflection nebulae and show gradual increases in their luminosity in the order of 6 magnitudes followed by a lengthy phase of constant brightness. They then dim by 2 magnitudes (six times dimmer) or so over a period of many years. V1057 Cygni for example dimmed by 2.5 magnitude (ten times dimmer) during an eleven year period. FU Orionis variables are of spectral type A through G and are possibly an evolutionary phase in the life of T Tauri stars.
In Main Sequence stars major eruptive variability is exceptional; it is common only among the heaviest (Wolf-Rayet) and the lightest (UV Ceti) stars.
Wolf-Rayet stars are massive hot stars that undergo periodic mass ejections causing them to brighten by 0.1 magnitude on average. They exhibit broad emission line spectra with helium, nitrogen, carbon and oxygen lines.
Flare stars, also known as the UV Ceti stars, are very faint main sequence stars, which undergo regular flares. They increase in brightness by up to two magnitudes (six times brighter) in just a few seconds, and then fade back to normal brightness in half an hour or less. Several nearby red dwarf stars are flare stars, including Proxima Centauri and Wolf 359.
Large stars lose their matter relatively easily. For this reason eruptivity is fairly common among giants and supergiants.
Also known as the S Doradus variables, the most luminous stars known belong to this class. Examples include the hypergiants η Carinae and P Cygni.
Gamma Cassiopeiae (γ Cas) variables are BIII-IVe type stars that fluctuate irregularly by up to 1.5 magnitudes (four-fold change in luminosity) due to the ejection of matter at their equatorial regions caused by a fast rotational speed.
While classed as eruptive variables, these stars do not undergo periodic increases in brightness; instead, they spend most of their time at maximum brightness. At irregular intervals, however, they suddenly fade by 1 - 9 magnitudes (2.5 to 4000 times dimmer), slowly recovering to their maximum brightness over months to years. This variation is thought to be caused by episodes of dust formation in the atmosphere of the star. As dust is formed and moves away from the star, it eventually cools to below the dust condensation temperature, at which point a cloud becomes opaque, causing the star's observed brightness to drop. The dissipating dust results in a gradual increase of brightness.
R Coronae Borealis (R CrB) is the prototype star. Other examples include Z Ursae Minoris (Z UMi) and SU Tauri (SU Tau). DY Persei variables are a subclass of R CrB variables that have a periodic variability in addition to their eruptions.
These are close binary systems with a longer period chromospheric activity, including flares, that typically last 1-4 years. This activity cycle is comparable to the solar cycle of the Sun. The type is often abbreviated RS CVn. The prototype of this class is also an eclipsing binary.
Supernovae are the most dramatic type of cataclysmic variable, being some of the most energetic events in the universe. A supernova can briefly emit as much energy as an entire galaxy, brightening by more than 20 magnitudes (over one hundred million times brighter). The supernova explosion is caused by a white dwarf or a star core reaching a certain mass/density limit, the Chandrasekhar limit, causing the object to collapse in a fraction of a second. This collapse "bounces" and causes the star to explode and emit this enormous energy quantity. The outer layers of these stars are blown away at speeds of many thousands of kilometers an hour. The expelled matter may form nebulae called supernova remnants. A well known example of such a nebula is the Crab Nebula, left over from a supernova that was observed in China and North America in 1054. The core of the star or the white dwarf may either become a neutron star (generally a pulsar) or disintegrate completely in the explosion.
Supernovae can result from the death of an extremely massive star, many times heavier than the Sun. At the end of the life of this massive star, a non-fusible iron core is formed from fusion ashes. This iron core is pushed towards the Chandrasekhar limit till it surpasses it and therefore collapses.
A supernova may also result from mass transfer onto a white dwarf from a star companion in a double star system. The Chandrasekhar limit is surpassed from the infalling matter. The absolute luminosity of this latter type is related to properties of its light curve, so that these supernovae can be used to establish the distance to other galaxies. One of the most studied supernovae is SN 1987A in the Large Magellanic Cloud.
Novae are also the result of dramatic explosions, but unlike supernovae do not result in the destruction of the progenitor star. Also unlike supernovae, novae ignite from the sudden onset of thermonuclear fusion, which under certain high pressure conditions (degenerate matter) accelerates explosively. They form in close binary systems, one component being a white dwarf accreting matter from the other ordinary star component, and may recur over periods of decades to centuries or millennia. Novae are categorised as fast, slow or very slow, depending on the behaviour of their light curve. Several naked eye novae have been recorded, Nova Cygni 1975 being the brightest in the recent history, reaching 2nd magnitude.
Dwarf novae are double stars involving a white dwarf star in which matter transfer between the component gives rise to regular outbursts. There are three types of dwarf nova:
These symbiotic binary systems are composed of a red giant and a hot blue star enveloped in a cloud of gas and dust. They undergo nova-like outbursts with amplitudes of some 4 magnitudes.
There are two main groups of extrinsic variables: rotating stars and eclipsing stars.
Stars with sizable sunspots may show significant variations in brightness as they rotate, and brighter areas of the surface are brought into view. Bright spots also occur at the magnetic poles of magnetic stars. Stars with ellipsoidal shapes may also show changes in brightness as they present varying areas of their surfaces to the observer.
These are very close binaries, the components of which are non-spherical due to their mutual gravitation. As the stars rotate the area of their surface presented towards the observer changes and this in turn affects their brightness as seen from Earth.
The surface of the star is not uniformly bright, but has darker and brighter areas (like the sun's solar spots). The star's chromosphere too may vary in brightness. As the star rotates we observe brightness variations of a few tenths of magnitudes.
These stars rotate extremely fast; hence they are ellipsoidal in shape.
BY Draconis stars are of spectral class K or M and vary by less than 0.5 magnitudes (70% change in luminosity).
Alpha-2 Canum Venaticorum (α2 CVn) variables are main sequence stars of spectral class B8 - A7 that show fluctuations of 0.01 to 0.1 magnitudes (1% to 10%) due to changes in their magnetic fields.
Stars in this class exhibit brightness fluctuations of some 0.1 magnitude caused by changes in their magnetic fields due to high rotation speeds.
Few pulsars have been detected in visible light. These neutron stars change in brightness as they rotate. Because of the rapid rotation, brightness variations are extremely fast, from milliseconds to a few seconds. The first and the best known example is the Crab Pulsar.
Extrinsic variables have variations in their brightness, as seen by terrestrial observers, due to some external source. One of the most common reasons for this is the presence of a binary companion star, so that the two together form a binary star. When seen from certain angles, one star may eclipse the other, causing a reduction in brightness. One of the most famous eclipsing binaries is Algol, or Beta Persei (β Per).
Algol variables undergo eclipses with one or two minima separated by periods of nearly constant light. The prototype of this class is Algol in the constellation Perseus.
Beta Lyrae (β Lyr) variables are extremely close binaries, named after the star Sheliak. The light curves of this class of eclipsing variables are constantly changing, making it almost impossible to determine the exact onset and end of each eclipse.
The stars in this group show periods of less than a day. The stars are so closely situated to each other that their surfaces are almost in contact with each other.
Stars with planets may also show brightness variations if their planets pass between the earth and the star. These variations are much smaller than those seen with stellar companions and are only detectable with extremely accurate observations. Examples include HD 209458 and GSC 02652-01324.
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