Stars are composed mainly of hydrogen and helium, with trace amounts of metals. They have extremely hot, dense cores which emit radiation in the form of a continuous spectrum (from the photosphere, the deepest layer which can be observed) which can be well approximated as a blackbody. This radiation then passes through the upper layers of the atmosphere, which are still hot but of lower density, and which absorb radiation preferentially at key wavelengths determined by the atomic composition of the atmosphere. The observed absorption lines depend primarily upon the exitation and ionization of the atmosphere, rather than its chemical composition.
We classify stars according to the characteristics of their spectral line features. Most differences (see this line plot, and these two-dimensional optical spectra) are caused by changes in temperature. A sub-class number (spectal type) further orders each alphabetic type from 0 (hottest) to 9 (coolest).
The spectral sequence (based on temperature): O B A F G K M L T
Spectral Class |
Color | Surface Temperature |
B-V Color |
Prominent Absorption Lines |
---|---|---|---|---|
O | Blue | 41,000o K | -0.32 | He+, O++, N++, Si++, He, H |
B | Blue | 31,000o K | -0.22 | He, H, O+, C+, N+, Si+ |
A | Blue-white | 9,500o K | 0.00 | H(strongest), Ca+, Mg+, Fe+ |
F | White | 7,240o K | +0.33 | H(weaker), Ca+, ionized metals |
G | Yellow-white | 5,920o K | +0.60 | H(weaker), Ca+, ionized and neutral metals |
K | Orange | 5,300o K | +0.81 | Ca+(strongest), neutral metals strong, H(weak) |
M | Red | 3,850o K | +1.41 | Strong neutral metals, TiO |
L | Red | 2,200o K | (+1.5) | Strong metal-hydride molecular bands, and H2O |
T | Red | 900o K | (+1.6) | Strong methane bands |
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[NMSU, N. Vogt] |
The MK spectral classification was originally based on the appearance of pairs of spectral lines in the blue region, at a resolution of 2A. Here are the critical ratios. Why do you think these data were used?
Class | Line pairs | |
---|---|---|
O5 - O9 | 4471 He I | 4541 He II |
B0 - B1 | 4552 Si III | 4089 Si IV |
B2 - B8 | 4129 Si II | 4121 He I |
B8 - A2 | 4471 He I | 4481 Mg II |
B8 - A2 | 4026 He I | 3934 Ca II |
A2 - F5 | 4032 Mn I | 4130 Mn I |
A2 - F5 | 4300 CH | 4385 CH |
F2 - K | 4300 Gband | 4340 H![]() |
F5 - G5 | 4045 Fe I | 4101 H![]() |
F5 - G5 | 4226 Ca I | 4340 H![]() |
G5 - K0 | 4144 Fe I | 4101 H![]() |
K0 - K5 | 4226 Ca I | 4325 Ca I |
K0 - K5 | 4290 Ca I | 4300 Ca I |
The secondary classification depends upon luminosity, and is designated by the Roman numerals I thru V, in order of decreasing luminosity:
Class | Name | Description |
---|---|---|
Ia | Bright supergiants | The brightest of the very massive and luminous stars, near the end of their lives. |
Ib | Supergiants | Very massive and luminous stars near the end of their lives (wide range of temperatures, narrow range of luminosities). Very rare - 1 in a million stars is a supergiant. |
II | Bright giants | Stars with a luminosity between giant and supergiant class. |
III | Giants | Mainly low-mass stars at the end of their lives that have swelled to become giants (large but cool); also some high mass stars evolving on their way to supergiant status. |
IV | Subgiants | Stars which have begun evolving to giant or supergiant status. |
V | Dwarfs | All normal hydrogen-burning stars; stars spend most of their lives in this category before evolving up the scale. O and B stars in this category are very luminous, brighter than most giants. |
(Main Sequence) |
How are spectral measurements of the following elements and molecules useful in determining temperatures, luminosities, and stellar composition: Ca, Mg, Na, H, CN, CH, MgH, CaH, TiO?
U | B | V | R | I | J | H | K | L | M |
3650 A | 4450 A | 5510 A | 6580 A | 8060 A | 1.22 u | 1.63 u | 2.19 u | 3.45 u | 4.75 u |