Search over 40,000 articles from the original, classic Encyclopedia Britannica, 11th Edition.
|
See also:STANZA (See also:Low See also:Lat. stantia, Ital. stantia or stanza) , properly an apartment or See also:storey in a See also:house, the See also:term being hence adopted for See also:literary purposes to denote a See also:complete See also:section, of recurrent See also:form, in a poem . . A See also:stanza is a See also:strophe of two or more lines, The See also:Greek is &drip, and the See also:Sanskrit See also:lava, for stara . The ultimate See also:root is unknown, but may be connected with that meaning " to strew," and the word would thus mean the points of See also:light scattered over the heavens . The study of the stars is coeval with the See also:birth of See also:astronomy (see ASTRONOMY: See also:History); and among the earliest civilizations beneficent or malevolent influences were as-signed to them (see See also:ASTROLOGY) . With the development of observational astronomy the sidereal universe was arbitrarily divided into areas characterized by See also:special assemblages of stars; these assemblages were named asterisms or constellations, and each received a name suggested by mythological or other figures . The heavenly bodies fall into two classes: (1) the fixed stars, or stars proper, which retain the same relative position with respect to one another; and (2) the See also:planets, which have motions of a distinctly individual See also:character, and appear to wander among the stars proper . Numerous See also:counts of the number of stars visible to the naked See also:eye have been made; it is doubtful whether more than 2000 can be seen at one See also:time from any position on the See also:earth . When a, See also:telescope is employed this number is enormously in-creased, and still more so with the introduction of photographic methods; with See also:modern appliances more than a See also:hundred million of these See also:objects may be rendered perceptible . The recognition of See also:star's is primarily dependent on their brightness or " magnitude "; and it is clear that stars admit of See also:classification on this basis . This was attempted Number and by See also:Ptolemy, who termed the brightest stars "of the Magnitude From the value of the light-ratio we can construct a table showing the number of stars of each magnitude which would together give as much light as a first magnitude star, viz.: I 21 6 16 40 See also:I00 Comparing these figures with the See also:numbers of stars of each magnitude we See also:notice that the See also:total light emitted by all the stars of a given magnitude is fairly See also:constant . Variable Stars.—Although the See also:majority of the stars are unchanging in magnitude, there are many exceptions . Stars whose brightness fluctuates are called variable stars . The number of known objects of this class is being added to rapidly, and now amounts to over 4000 . The systematic See also:search made at Harvard See also:Observatory is responsible for a large proportion of the See also:recent discoveries . Many of these stars seem to vary quite irregularly; the changes of magnitude do not recur in any orderly way . Others, however, are periodic, that is to say, the sequence of changes is repeated at See also:regular intervals, and it is thus possible to predict when the maximum and minimum brightness will occur . Of the periodic variable stars, the lengths of the periods range from 3 See also:hours 12 minutes, which is the shortest yet determined, to 6,o days, the longest . When See also:statistics of the lengths of the periods are collected, it is at oncenoticed that they fall into two fairly well-marked classes . The following table, based on S . C . See also:Chandler's "Third See also:Catalogue" (Astronomical See also:Journal, vol. xvi.)," supplemented by A . W . See also:Roberts's See also:list of See also:southern variables (ibid. vol. xxi.), classifies the lengths of the periods of 330 stars . It will be noticed that there are very few periods between 50 and 15o days, that a considerable number are less than 5o days (actually a large majority of these are less than to days), and that from 150 days upwards the number of periods increases to a maximum at about 350 days and then diminishes .
We thus recognize two classes of variables, of which (I) the See also:long-See also:period variables have periods ranging in See also:general from 15o to 450 days, though a few are outside these limits; and (2) the See also:short-period variables have periods less than 5o days (in the majority of cases less than lo days)
.
There is some over-lapping of these two classes as regards length of period, and it is doubtful in which class some stars, whose periods are between lo days and 150 days, should be placed; but the two classes are quite distinct physically, and the variability depends on entirely different causes
.
Long-period Variables.—The best known and typical star of this class is Mira or o Ceti
.
This was the first variable star to be discovered, having been noticed in 1596 by See also:David See also:Fabricius, who thought it was a new star (a Nova)
.
The varying brightness, ranging from the ninth to the second magnitude, was recognized in 1639 by See also: The spectrum is of the third type with See also:bright See also:hydrogen emission lines (see below, Spectra of Stars) . Stars having this type of spectrum are always variable, and a large proportion of the more recently discovered long-period variables have been detected through their characteristic spectrum . x Cygni is another star of this class, remarkable for its range of magnitude . In its period of 406 days it fluctuates between the thirteenth and the See also:fourth magnitudes; thus at maximum it emits 4000 times as much light as at minimum . The mean range of 75 long-period variables observed at Harvard (Harvard See also:Annals, vol . Ivii.) was five magnitudes . Another variable, R Normae L is of See also:interest as having a pronounced See also:double maximum in each period . It is natural to compare the periodic outbursts occurring in these stars with the outbursts of activity on the See also:sun, which have a period of about eleven years . In both cases no extraneous cause can be assigned; the period seems to be inherent in the star itself and not to be determined by the revolution of a See also:satellite (no variability of the See also:line-of-sight See also:motion of Mira has been found, so that it is probably not accompanied by any large See also:companion) . In both cases the rise to a maximum is more rapid than the decline to a minimum, and in fact some of the See also:minor peculiarities of the sunspot See also:curve are closely imitated by the light-curves of variable stars . H . H . See also:Turner has analysed harmonically the light-curves of a number of long period variables, and has shown that when they are arranged in a natural See also:series the sun takes its place in the series near, but not actually at, one end . It is necessary to suppose, if the See also:analogy is to hold, that the sun is brightest when sunspots and faculae are most numerous; this is by no means unlikely . On the other See also:hand, the See also:variations in the light of the sun must be very small compared with the enormous fluctuations in the light of variable stars . Moreover, the See also:solar period (II years) is far outside the limits of the periods of 1 Variable stars (except those sufficiently bright to have received special names) are denoted by the See also:capital letters R to Z followed by the name of the See also:constellation . The first nine variables recognized in each constellation are denoted by single letters, after which combinations RR, RS, &c:, are used . 1st mag . 14 2nd mag . 3rd mag . 4th mag . 5th mag . 6th mag . 20I0 152 48 854 313 1st mag . 2nd mag . 3rd mag . 4th mag . 5th mag . 6th mag . 0/the Stars. first magnitude," and the progressively fainter of the S stars of progressively greater magnitude . Ptolemy's classification has been adopted as the basis of the more exactly quantitative modern See also:system . In this system one star is defined to be unit magnitude higher than another if its light is less in the ratio 1:2.512 . This ratio is adopted so that a difference of five magnitudes may correspond to a light-ratio of 1 : too . This subject is treated in the See also:article See also:PHOTOMETRY, See also:CELESTIAL . The faintest stars visible to the naked eye on clear nights are of about the See also:sixth magnitude; exceptionally keen, well-trained eyes and clear moonless nights are necessary for the See also:perception of stars of the seventh magnitude . According to E . Heis the numbers and magnitudes of stars between the See also:north See also:pole and a circle 350 See also:south of the See also:equator are: Period o 50 See also:loo 150 200 250 300 350 400 450 5o0 550 600 in to to to to to to to to to to to to to days 50 100 15o 200 250 300 350 400 450 500 550 600, 650 Stars 73 8 12 22 41 45 49 50 20 6 I 2' I variables . It is therefore perhaps misleading actually to class the sun with them; but it seems highly probable that whatever cause produces the periodic outbursts of spots and faculae on our sun differs only in degree from that which, in stars under a different physical See also:condition of pressure and temperature, results in the gigantic conflagrations which we have been considering . Short-period Variables.—Besides the shortness of the period these variables possess other characteristics which differentiate them from the long-period variables . The range of variation is much smaller, the difference between maximum and minimum rarely exceeding two magnitudes . Also the variations recur with perfect regularity . There is See also:reason to believe that all the stars of this class are binary systems, and that the variations of brightness are deter-See also:mined by the different aspects presented by the two component stars during the period of revolution . There are several well-marked varieties of short-period variables; the most important are typified by the stars See also:Algol, 13 Lyrae, I- Geminorum and S Cephei . In the Algol variables one of the component stars is dark (that is to say, dark in comparison with the other), and once in each revolution, passing between us and the bright component, partially hides it . This class of variables is accordingly characterized by the fact that for the greater See also:part of the period the star shines steadily with its maximum brilliancy, but fades away for a short time during each period . The variability of Algol ($ Persei) was discovered in 1783 by John Goodricke (1764–1786), but, judging from its name, which signifies " the demon," it seems possible that its peculiarity may have been known to the See also:ancient astronomers . Algol is ordinarily of magnitude 2.3, but once in a period of 2d . 2oh . 49m. it suffers partial See also:eclipse and fades to magnitude 3'5 . The duration of each eclipse is 91 hours . Ever since the variability of Algol was observed it was suspected to be due to a partial eclipse of the star by a dark See also:body nearly as large as itself revolving See also:round it; but the explanation remained merely a surmise until K . H . See also:Vogel of See also:Potsdam, by repeated measurements of the motion of Algol in the line of sight, showed that the star is always receding from us before the loss of light and approaching us afterwards . This leaves no See also:room for doubt that an invisible companion passes between us and Algol about the time the diminution of light takes place, and so proves the correctness of the explanation . The dimensions of the Algol system have been calculated, with the result that Algol appears to have:a See also:diameter of 1,000,000 m. and its companion a diameter of 830,000 m.; the distance between their centres cannot be deduced without making certain doubtful assumptions, but may be about 3,000,000 m . When this distance is compared with those prevailing in the solar system, it seems an extraordinarily small separation between two such large bodies; we shall, however, presently come across systems in which the two components revolve almost or actually in contact . About 56 Algol variables were known in 1907; the variables of this class are the most difficult to detect, for the short period of obscuration may easily See also:escape notice unless the star is watched continuously . The variable star Lyrae, which is typical of another class, was also discovered by Goodricke in 1784 . It differs from the Algol type in having two unequal minima separated by two equal maxima . Thus in a period of 12d . 22h• from a maximum of magnitude 3.4 it falls to 3.9, rises again to 3.4, then falls to 4.5 and returns to magnitude 3.4 . The changes take place continuously, so that there is no period of steady luminosity . The See also:hypothesis of G . W . See also:Myers (Astrophysical Journal, vol. vii.) affords at least a partial explanation of the phenomena . Two stars are supposed to revolve about one another nearly or actually in contact . In such a system the tidal forces must be very See also:great, and under their See also:influence the stars will not be spherical, but will be elongated in the direction of the line joining their centres . When the line of centres is at right angles to our line of sight, the stars See also:present to us their greatest apparent See also:surface, and therefore send us the maximum light . This happens twice in a revolution . As the line of centres becomes more oblique, the surface is seen more and more foreshortened and the brilliancy diminishes continuously . Supposing that the two stars are of unequal surface brilliancy, the magnitude at minimum will depend on which of the two stars is the nearer to us, accordingly there are two unequal minima in each revolution . When the two stars are of equal brilliancy the minima are equal; this is the See also:case in variables of the Geminorum type . When the orbits are See also:eccentric, the tidal disturbance varying with the distance between the two components will probably cause changes in their See also:absolute brilliancy; the variation due to change in the aspect of the system presented to us may thus be supplemented by a real See also:intrinsic variation, both, however, being regulated by the orbital motion . A large eccentricity also produces an unsymmetrical light 'variation, the minimum occurring at a time not midway between two maxima ; stars. of this character are called Cepheid variables, after the typical star S Cephei . All the best-known short-period variables have been proved to be binary systems spectroscopically, and to have periods corresponding with the period of light variation, so that to this extent the hypothesis we have described is well founded; but it is doubtful if it is the whole explanation . S . Albrecht has shown that, of the 10 members of the S Cephei class for which both the orbits and the light-variations are thoroughly known, the maximum light always occurs approximately at the time when the brightercomponent is approaching us most rapidly; this relation, which seems to be well established, is a most perplexing, one . No hard and fast physical distinction can be See also:drawn between the various classes of short-period variables; as the distance between the components diminishes the Algol variable merges insensibly into the ti Lyrae type . The latter, on the other hand, is perhaps connected by insensible gradations with the See also:ordinary See also:simple star . See also:Sir G . H . See also:Darwin and H . See also:Poincare have investigated the forms taken up by rotating masses of fluid . When the angular momentum is too great for the usual spheroidal form to persist, this gives place to an See also:ellipsoid with three unequal axes; this is succeeded by a See also:pear-shaped form . The subsequent sequence of events cannot be traced with certainty, but it seems likely that the pear-shaped form is succeeded by an See also:hour-See also:glass-shaped form, which finally separates at the See also:neck into two masses of fluid . Ellipsoidal, pear-shaped or hour-glassshaped stars would all give rise to the phenomena of a short-period variable, and doubtless examples of these intermediate forms exist . Certain clusters contain a remarkable number of short-period variables . Thus the cluster Messier 5 was found at Harvard to contain 185 variables out of 9900 stars examined . See also:Solon I . See also:Bailey, on examining 63 of them, found that with one exception their periods See also:lay between 1oh . 48m. and 14h . 59.., and the range of variation between 0.7 and 1.4 magnitudes . Moreover, the light-curves were all of a See also:uniform type, a distinctive feature of " cluster variables " being the rapid rise to a maximum and slow decline . Temporary Stars or Novas.—From time to time a star, hitherto too faint to be noticeable, blazes out and becomes a prominent See also:object, and then slowly fades into obscurity . According to See also:Miss See also:Agnes See also:Clerke there are records of. ten such stars appearing between 134 B.C. and A.D . 1500 .
Since that time nine novas have appeared, which have attained naked-eye visibility; and in recent years a number of very faint objects of the same class have been detected
.
The brightest star of all these was the famous " Tycho's star " in See also:Cassiopeia
.
It was first observed on the 6th of See also:November 1572 by Wolfgang Schuler
.
In five days its light had reached the first magnitude, and a little later it even equalled See also:Venus in brilliancy and was observed in full daylight
.
After three See also:weeks it began to decline, but the star did not finally disappear until See also: In See also:July 1903 it was of the twelfth magnitude, and its light has remained constant since then . In the case of this star there is See also:evidence that the outburst must have been extremely rapid, for the region where Nova Persei appeared had been photographed repeatedly at Harvard during February, and in particular no trace of the star was found on a See also:plate taken on the 19th of February, which showed See also:eleventh magnitude stars . Thus a rise of at least eight magnitudes in two days must have occurred . On the 21st of See also:August, six months after the See also:discovery of Nova Persei, C . Flammarion and E . M . Antoniadi discovered that a nebula surrounded it.' Subsequent photographs showed that this nebula, which consisted mainly of two incomplete rings of nebulosity, was expanding outwards at the See also:rate of from 2" to 3" per See also:day . This expansion continued at the same rate until the following year . Spectroscopic examination had already suggested prodigious' velocities of the See also:order of 100o m. per second in the gases of the See also:atmosphere of the nova; but the velocity implied by this expansion of the nebula was unprecedented and comparable only with the velocity of light . The See also:suggestion was made, and seems to be the true explanation, that what was actually witnessed was the See also:wave of light due to the outburst of the nova, spreading outwards with its velocity of 186,000 m. per second, and rendering luminous as it reached them the particles of a pre-existing nebula, whose own light had been too faint to be visible . Two possible explanations of the phenomena of temporary stars have been held . The collision theory supposes that the outburst is the result of a collision between two stars or between a star and a swarm of meteoric or nebulous See also:matter . The See also:explosion theory regards the outburst as similar to the outbreak of activity of a long-period variable . Probably the latter hypothesis is the one more generally accepted now . There is one unique star, which is of special interest as occupying rather an intermediate position between a nova and a long-period variable . This is the southern star ri See also:Argus (sometimes called n Carinae) . From 1750 until about 1832 it seems to have varied irregularly between the second and the fourth magnitudes . For the next ten years it slowly increased (though with slight check), and in 1843 was nearly as bright as Sirius; since then it has slowly faded, but it was not till 1869 that it ceased to be visible to the naked eye . It is now about magnitude 7.5 . The slowness both of the rise and decline is in great contrast with the Double Stars cases the proximity is only apparent; one star may . be really at a vast distance behind the other, but, being in the same line of See also:vision, they appear See also:close together . In many cases, however, two or more stars are really connected, and their distance from one another is (from the astronomical standpoint) small . The evidence of this connexion is of two kinds . In a number of cases See also:measures of the relative positions of the two stars, continued for many years, have shown that they are revolving about a See also:common centre; when this is so there can be no doubt that they form a binary system, and that the two components move in elliptic orbits about the common centre of See also:mass, controlled by their mutual See also:gravitation . But these cases form a very small proportion of the total number of double stars . In many other double stars the two components have very nearly the same proper motion . Unless this is a See also:mere coincidence, it implies that the two stars are nearly at the same distance from us . For otherwise, if they had from some unknown cause the same actual motion, the apparent motion in arc would be different . We can therefore infer that the two stars are really comparatively close together, and, moreover, since they have the same proper motion, that they remain close together . They may thus be fairly regarded as constituting a binary system, though the gravitational attraction between some of the wider pairs must be very weak . Several double stars were observed during the 17th See also:century, Ursae Majoris being the first on See also:record . In 1784 See also:Christian See also:Mayer published a catalogue of all the double stars then known, which contained 89 pairs . Between 1825 and 1827 F . G . W . See also:Struve at Dorpat examined 120,000 stars, and found 3112 double stars whose distance apart did not exceed 32" . W . S . Burnham's General Catalogue of Double Stars (1907) contains 13,655 pairs north of See also:declination -31 ° . Undoubtedly a large number of these are only See also:optical pairs, but mere considerations of See also:probability show that the majority must be physically connected . For only 88 of them has it been possible as yet to deduce a period, and at least half even of these periods are very doubtful . The rates of motion are so slow that many centuries' observations are needed to determine the See also:orbit . The most rapid visual binary (leaving aside See also:Capella for the moment) is b Equulei, which completes a 'See also:evolution in 5.7 years . Next to it come 13 Ceti, period 7.4 years, and K Pegasi, period 11.4 years . From a list of systems with determined periods given by Aitken (Lick Observatory Bulletin, No . 84) there are 20 with periods less than 5o years, and 16 between 5o and too years . S Equulei, 13 Ceti and K Pegasi are all extremely close pairs, and can only be resolved with the most powerful See also:instruments . Capella, whose period is only 104 days, was discovered to be double by means of the spectroscope, but has since been measured frequently as a visual binary at See also:Greenwich . With the best instruments a star can be distinguished as double when the separation of the two components is a little less than o• 1 " . From the very few orbits that have as yet been determined one interesting result has been arrived at . Most of the orbits are remarkably eccentric ellipses, the See also:average eccentricity being about o.5 . There is a very striking relation between the eccentricity and the period of a system; in general the binaries of longest period have the greatest eccentricities . The relation applies not only to the visual but to the spectroscopic binaries; these, having shorter periods than the visual binaries, have generally quite small eccentricities . Another interesting feature is that, where the two components differ in brightness, the fainter component is often the one possessing the greater mass . Far within the limit to which telescopic vision can extend binary systems are now being found by the spectroscope . These systems Spectre- appear as a connecting See also:link between short-period ed variable stars on the one hand and telescopic double scopic Btaaries. stars on the other . Stars of the class to which the Algol type of variables belongs will appear to us to vary only in the exceptional case when the See also:plane of the orbit passes so near our sun that one body appears to pass over the other and so causes an eclipse . Except when the line of sight is perpendicular to the plane of the orbit, the revolution of the two bodies will result in a periodic variation of the motion ;n the, line of sight . Such a variation can be detected by the spectroscope . If both the bodies are luminous, especially if they do not differ much in brilliancy, the motion of revolution is shown by a periodic doubling of the lines of the spectrum; when one body is moving towards us and the other away their spectral lines are displaced (according to Doppler's principle) in opposite directions, so that all the lines strong enough to appear in both spectra appear double; when the two bodies are inconjunction, and therefore moving transversely, their spectra are merged into one and show nothing unusual .
More usually, however, only one component is sufficiently luminous for its spectrum to appear; its orbital motion is then detected by a periodic change in the absolute displacement of its spectral lines
.
Up to 1905, 140 spectroscopic binaries had been discovered ; a list of these is given in the Lick Observatory Bulletin, no
.
79
.
Details of the calculated orbits of 63 spectroscopic binaries are given in Publications of the See also:Allegheny Observatory, vol. i
.
No
.
21
.
According to W
.
W
.
See also: Tidal See also:action also accounts for the progressively increasing eccentricities of the orbits, already referred to . This theory of the See also:genesis of double-stars by fission is not, however, universally accepted; in particular objections have been urged by T . C . Chamberlin and F . R . See also:Moulton . It is true that rotational instability alone is not competent to explain the separation into two components; but the existence of gravitational instability, pointed out by J . H . Jeans, enables the See also:principal difficulties of the theory to be surmounted . Whilst there is thus no well-defined See also:lower limit to the dimensions of systems of two stars, on the other hand we cannot set any See also:superior limit either to the number of stars which shall form a system or to the dimensions of that system . No star is altogether removed from the attractions of its neighbours, and there are cases where some sort of connexion seems to relate stars which are widely separated in space . A curious case of this sort is that of the five stars 13, y, 5, e and of Ursa See also:Major . These have proper motions which are almost identical in amount and in direction . The agreement is too close to be dismissed as a mere coincidence, and it is confirmed by a corresponding agreement of. their radial motions determined by the spectroscope; and yet, seeing that /3 and i' Ursae Majoris are 19° apart, these two stars must be distant from each other at least one-third of the distance of each from the sun; thus the members of this singular See also:group are separated by the ordinary stellar distances, and probably each has neighbours, not belonging to the system, which are closer to it than the other four stars of the group . Further, E . Hertzsprung has shown that Sirius also belongs to this same system and shares its motion, notwithstanding that it is in a nearly opposite part of the See also:sky . It is difficult to understand what may be the connexion between stars so widely separated ; from the equality of their motions they must have been widely separated for a very long period . Of multiple stars the most famous is e Orionis, situated near the densest part of the great See also:Orion nebula . It consists of four principal stars and two faint companions . From the more complex star. systems of this See also:kind, we pass to the See also:consideration of star- Clusters. clusters, which are systems of stars in which the components are very numerous . When examined with a telescope of See also:power insufficient to separate the individual stars, a cluster appears like a nebula . The " beehive cluster " Praesepe in See also:Cancer is an example of an easily resolved See also:Ouster composed of fairly bright stars . The great cluster in See also:Hercules (Messier 13), on the other hand, requires the highest telescopic power for its complete See also:resolution into stars . Doubtless with improved telescopes many more apparent nebulae would be shown to be clusters, but there are certainly many nebulae which are otherwise constituted . Many of the clusters are 'of very irregular forms, either showing no well-marked centre of condensation, or else condensed in streams along certain lines . There is, however, a well-marked type to which many of the richest clusters belong; these are the globular clusters . They have a symmetrical circular shape, the condensation increasing rapidly towards the centre . The Hercules cluster is of this form; another example is w Centauri, in which over 6000 stars have been counted, comprised within a circle of about 40' diameter . These clusters present many unsolved problems . Thus Perrine, from an examination of ten globular clusters (including Messier 13 and w Centauri), has found in each case that the stars can be separated into two classes of magnitudes . About one-third of the stars are between magnitudes 11 and 13, and the remaining two-thirds are between magnitudes 15.5 and 16.5 . Stars of magnitudes intermediate between these two See also:groups are almost entirely absent . Thus each cluster seems to consist of two kinds of stars, which we may distinguish as bright and faint; the bright stars are all approximately of one See also:standard See also:size, and the faint stars of another standard size and brightness . The question of the stability of these clusters is one of much interest . The mutual gravitation of a large number of stars crowded in a comparatively small space must be considerable, and the individual stars must move in irregular orbits under their mutual attractions . It does not seem probable; however, that they can escape the See also:fate of ultimately condensing into one confused mass .
If this surmise be correct, we are witnessing in clusters a See also:counter-See also:process of
progress of a nova. n Argus is surrounded by a nebula, the famous " Keyhole nebula "; in this respect it resembles Nova Persei
.
System of Stars.—On examining the stars telescopically, many which appear single to the unaided eye are found to be composed of two or more stars very close together
.
In some
evolution to that which is taking place in double stars; the latter appear to be separating from a single See also:original mass and the former condensing into one
.
See also:Colours and Spectra of Stars.—The brighter stars show a
marked variety of See also:colour in their light, and with the aid of a
telescope a still greater diversity is noticeable
.
It is,
Colours
.
however, only the red stars that form a clearly marked class by themselves
.
For purposes of precise scientific investigation the study of spectra is generally more suitable than the vague and unsatisfactory estimates of colour, which differ with different observers
.
Of the first magnitude red stars Antares is the most deeply coloured, Betelgeux, Aldebaran and See also:Arcturus being successively less conspicuously red
.
Systematic study of red stars See also:dates from the publication in 1866 of Schjellerup's Catalogue, containing a list of 28o of them
.
The two components of double stars often exhibit complementary colours
.
As a See also:rule contrasted colours are shown by pairs having a bright and a faint component which are relatively wide apart; brilliant See also:
The occurrence of change, either periodic or irregular, in the colour of individual stars, has been suspected by many observers ; but such a colour-variability is necessarily very difficult to establish
.
A possible change of colour in the case of Sirius is noteworthy
.
In modern times Sirius has always been a typical white or bluish-white star, but a number of classical writers refer to it as red or fiery
.
There is perhaps room for doubt as to the precise significance of the words used; but the fact that Ptolemy classes Sirius with Antares, Aldebaran, Arcturus, Betelgeux and Procyon as " fiery red " (UebKnp,doi) as compared with all the other bright stars which are " yellow " (favOoc) seems almost conclusive that Sirius was then a redstar
.
When examined with the spectroscope the light of the stars is found to resemble generally that of the sun
.
The spectrum consists Spectra of of a continuous See also:band of light crossed by a greater or Stara: less number of dark absorption lines or bands
.
As in
the case of the sun, this indicates an incandescent body which might be solid, liquid, or a not too rare See also:gas, surrounded by and seen through an atmosphere of somewhat cooler gases and vapours; it is this cooler envelope whose nature the spectroscope reveals to use and in it the presence of many terrestrial elements has been detected by identifying in the spectrum their characteristic absorption lines
.
Stellar See also:spectroscopy dates from 1862, when Sir See also: Secchi's Type I. or " Sirian " type includes most of the bright white stars, such as Sirius, See also:Vega, Rigel, &c.; it is characterized by strong broad hydrogen lines, which are often the only absorption lines visible . Type II. includes the " Solar " stars, as Capella, Arcturus, Procyon, Aldebaran, their spectra are similar to that of the sun, being crossed by very numerous See also:fine lines, mostly due to vapours of metals . The great majority of the visible stars belong to these first two types . Type III. or " Antarian ' stars are of a reddish colour, such as Antares, Betelgeux, Mira, and many of the long-period variables . The spectrum, which closely resembles that of a sunspot, is marked by flutings or hands of lines sharply bounded on the violet See also:side and fading off towards the red . It has been shown by A . See also:Fowler that these flutings are due to See also:titanium See also:oxide; this probably indicates a relatively See also:low temperature, for at a high temperature all compounds would be dissociated . Type IV. also consists of red stars with banded spectra, but the bands differ in arrangement and See also:appearance from those in the third type, and are sharply bounded on the red side . These stars are also believed to have a comparatively low surface temperature, and the bands are attributed to the presence of compounds of See also:carbon . About 250 Type IV. stars are known, but none conspicuous; 19 Piscium, the brightest, is of magnitude 5.5 . Other classifications which are extensively used are those respectively of K . H . Vogel, J . N . See also:Lockyer and the See also:Draper Catalogue . The divergences depend mainly on the different views taken by their authors as to the order of stellar evolution . Apart from these considerations, the chief modification in the classification introduced by more recent investigators has been to separate Secchi's Type I. into two divisions, called See also:helium and hydrogen stars respectively . The former are often called " Orion " stars, as all the brighter stars in that constellation with the exception of Betelgeux belong to the helium type . Helium stars are generally considered to be the hottest and most luminous (in proportion to size) of all the stars . Type II. is now subdivided into." Procyon," " Solar " and " Arcturian ' stars, The " Procyon "or See also:calcium stars form a transition between Type I. and Type II. proper, and show the lines of calcium besides those of hydrogen . An important variety of Type III. spectra has been recognized, in which, as well as the usual absorption bands, bright emission lines of hydrogen appear; stars having this particular spectrum are always variable . Finally, a fifth type has been added, the See also:Wolf-Rayet stars; these show a spectrum crossed by the usual dark lines and bands, but showing also bright emission bands of blue and yellow light . About See also:ioo Wolf-Rayet stars are known, of which y Velorum is the brightest ; they are confined to the region of the Milky Way and the Magellanic Clouds . (See See also:PLANET.) Evolution of Stars.—The See also:absence of the distinctive lines of an See also:element in the spectrum does not by any means signify that that element is wanting or scarce in the star . The spectroscope only yields See also:information about the thin See also:outer envelope of the star; and even here elements may be present which do not reveal themselves, for the spectrum shown depends very greatly on the temperature and pressure . Stars of the different types are therefore not necessarily of different chemical constitution, but rather are in different physical conditions, and it is generally believed that every star in the course of its existence passes through stages corresponding to all (or most of) the different types . The stars are known to be continually losing enormous quantities of See also:energy by radiating their heat into space . Ordinary solid or liquid masses would cool very rapidly from this cause and would soon cease to shine . But a globe of gaseous matter under similar conditions will continually See also:contract in See also:volume, and in so doing transforms potential energy into heat . It was shown by See also:Homer |