Astronomy 2022 October 17-19

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1
color
spectral property of stars, the most basic one, determined by the light emitted at a specific peak wavelength. Explained by Wein’s law and related to temperature
2
spectra
spectral property of stars, Photosphere of a star is surrounded by a thin, hot atmosphere, dark line spectrum, Kirchoff’s third law
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stars
hot, dense balls of incandescent gas, follow Kirchoff’s first law: they emit a continuous spectrum
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photosphere
the part of the star you see with your naked eye. The color you see is explained by Wein’s law. Below this level, the stars are opaque, and above, the star’s atmospheres are transparent.
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temperature
depends on either temperature of photosphere, core, or envelope of a star
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luminosity
based on temperature and surface area; Stefan Boltzmann law
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spectrograph
classifying by spectral types/spectra, can be used to break star’s light into a continuous and absorption spectrum
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absorption spectrum/lines
can be used to determine temperatures and/chemical compositions of stars, lines dark due to absorption of light at specific wavelengths, can be used to identify elements of a star’s outer atmosphere
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Angelo Secchi
1866, classified stars into four main classes based on spectral lines
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Annie Jump Cannon
Harvard computer, noticed stellar temperature was the distinguishing spectral feature. Reordered types by temperature and most old classes were thrown out, analyzed and classified 220k stars
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Cecilia Payne-Gaposchkin
proposed stars were 80% hydrogen, 19% helium, 1% metal, and that most spectral lines came from different ionization states of same elements/created by different temperatures
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O and B stars
10,000k-50,000k, most hydrogen is ionized, only very weak hydrogen lines since there aren’t many electrons to make absorption lines
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A and F stars
7,500k-10,000k, ideal excision conditions, strongest hydrogen lines
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G, K, and M stars
5,000k-6,000k, cool temperatures, limited ionization, weak hydrogen lines because electrons are in a ground state
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spectral classification
classifications of stars by temperature, OBAFGKM hot-cool
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spectral subclass
OBAFGKM sequence later updated by subdividing each spectral type with numbers 0-9
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O stars
blue, temp 30k-50k K, luminosity 100k+ L, mass 3-20m, life expectancy 1-500Myr
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B stars
blue/white, mass 3-20m, temperatures 10k-30k K, luminosity 100-100k L, life expectancy 1-500 Myr
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A stars
white, mass 1.5-3m, temperatures 7.5k-10k k, luminosity 10-100 L, life expectancy 500-3Gyr
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F stars
yellow/white, mass 1.2-1.5m, temperatures 6k-7.5k K, luminosity 3-10 L, life expectancy 3-6 Gyr
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G stars
yellow, mass .85-.1.2 M, temperatures 5k-6k K, luminosity .5-3 L, life expectancy 6-15 Gyr
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K stars
yellow/orange, mass .5-.85M, temperature 3.8k-5k K, luminosity .01-.5 L, life expectancy 15-60 Gyr
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M stars
red, mass .075-.5m, temperature less than 3.8k K, luminosity less than .01 L, life expectancy 60Gyr-6Ty
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brown dwarf
L, T, Y, failed stars
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distribution of stars by mass
For every 1 O star there are 4.4k b stars, 20k A stars, 100k F star, 250k G stars, 400k K stars, 2.5m M stars
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Pickering and Fleming
classified 10k stars by strength of absorption lines A-O, strongest to weakest hydrogen lines, Harvard observatory used objective prism to collect spectra of 220k stars
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spectral classes
assigned by strengths or absence of specific spectral lines, sensitive to pressure and density in atmosphere
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classification by temperature
classification, color is determined by surface temperature, range 18k K- 60k K
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classification by luminosity
classifications of stars determined by width/mass, range 1/10k L to 6M L, .07 m-315 m
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range of radii/mass
.07 m-315 m, .8 R-2,150 R
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luminosity radius temperature relationship
luminosity, the total energy output of a star, depends on the temperature of photosphere T, and the surface area of photosphere determined by radius
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Stefan Boltzmann law
luminosity of a star proportiona to the fourth power and it’s radius squared, explains luminosity radius temperature relationship, L=r^2 T^4
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Morgan Keenan luminosity classes
1a-0: extremely luminous supergiants
1a: brightest supergiants
1b: less luminous supergiants
11: bright giants
111: giants
1V: subgiants (intermediate)
V: main sequence dwarfs (m-s
34
stellar densities
density of a star is mass/volume (4/3piR^3). Main sequence stars: range of average densities, giants low densities (10^-7 g/cc), supergiants very low density (10^-9 g/cc), white dwarfs high density (10^-5 g/cc)
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spectral lines
sensitive to pressure and density, determines luminosity classes, large stars have narrow lines and low pressure atmospheres, small stars have broader lines and high pressure atmospheres
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main sequence stars
OBAFGKM, 85% of stars lie along diagonal the band in HR diagram, luminosity .05-700k, temperature 3k to 40k, radius .6 to 18, mass .1-40
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giants
mostly K and M, same temperature as main sequence but brighter and larger, 6k-2k K, luminosity 1k-100k, low density stars 10^-7 g/cc
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supergiants
mostly K and M, largest stars with wide range of temperatures and luminosity, radius 20-2.15k R, luminosity 100k-6M, very low density 10^-9 g/cc
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white dwarf
white hot and small, much fainter than main sequence but same temperature, radius .01r (earth size), temperature 60k kelvin, luminosity .005 L, high density 10^-5 g/cc
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