05spectralclasses
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Transcript 05spectralclasses
Classification of Stellar Spectra
Late 1800s: first high-quality spectral measurements of stars
What are the main features – and how to classify them?
Spectral Lines
• Balmer absorption lines occur
when an incoming photon
causes an electron in the n = 2
level in hydrogen to jump to a
higher level.
• The hotter a star, the more likely
that hydrogen electrons will be
in the n = 2 level
• But for very hot stars, hydrogen
will lose its electrons completely
• Balmer lines thus reach their
maximum “depth” in the spectra
of stars with T=9250 K, so let’s
call those stars class ‘A’
Balmer
emission
series
Dependence of Spectral Lines vs.
Temperature
Stellar Spectral Lines
• Why do spectral lines
depend upon temperature?
– Populations of various
atomic states depends
upon temperature
• Degeneracy of levels
– Stage of ionization
• Depends on Pressure and
density…
• Depends somewhat on
composition of star as well
The Spectral Sequence
• In 1890, Edward Pickering and
his assistant at Harvard
classified thousands of stellar
spectra at Harvard.
• Named them ‘A’ through ‘Q’
based on Balmer depth.
• Approx. 20 years later,
blackbody theory was
developed.
• A. Cannon ‘improved’ the
scheme and re-ordered it by
temperature: O,B,A,F,G,K,M
• Subdivided each into 0 through
9 (AO: hot – A9:cooler)
• Later on, L and T were added.
E. Pickering and his
housekeeper W. Fleming
A. J. Cannon classifying one of
200,000 spectra by eye for 25¢ an
hour ($6 today)
Spectral Type Classification System
O B A F G K M (L T)
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50,000 K
1,000 K
Temperature
The Spectral Sequence and Temperature
Cecilia
PayneGaposchkin
40000 K
20000 K
“Stars”
9000 K
7000 K
Our sun: G2
5500 K
4500 K
3000 K
“Brown
dwarfs”
(no H fusion)
2000 K
< 1300 K
Hertzsprung-Russell diagram
• In early 1900s, H. Russell and E.
Hertzsprung independently
plotted absolute V magnitude
against spectral class
• Most stars fall along a band
(main sequence)
• Some are very luminous
compared to main sequence
stars of their spectral class
(implied large radius) giants
• Some are very underluminous
for their class white dwarfs
Star with Hipparcos
parallax distance
measurements
Note multiple axis
labels
HR Diagram from Gaia Parallax
Measurements
Stellar Luminosity Classes
• In 1930s, W. Morgan and P. Keenan noticed that stars with the
same temperature could have different Balmer absorption depths.
• Called the narrowest ones I and the deepest ones VI
A0 I
A0 II
A0 V
Spectra of three A0 stars of different luminosity class
Origin of Luminosity Classes
• At higher pressure, the gas particles in a stellar atmosphere are
closer together and can interact more frequently.
• The energy levels of the atoms are perturbed, so that a wider
range of photon frequencies can be absorbed.
Narrow line,
low density
pressure
Pressure broadening of a CO2
absorption line
Morgan-Keenan Luminosity classes
Betelgeuse
Arcturus, Capella
Most common type
(includes our Sun)
Sirius B
Morgan-Keenan Luminosity classes
Recall that luminosity
class varies with
surface gravity, which
varies as M / R2
Leads to luminosity
class regions on the
H-R diagram
Hertzsprung-Russell diagram
•
Stefan-Boltzmann law gives lines of constant radius:
Main Sequence Relations
Higher luminosity higher mass higher temp shorter
lifetime
Note the
increasing
mass and
shorter
lifetimes as you
climb the main
sequence
Stars leave the
main sequence
toward the end
of their lives
Spectroscopic Parallax Method
• Can use H-R diagram to
estimate absolute magnitude
of star given its spectral type
and luminosity class
• Use apparent magnitude and
distance modulus formula:
• Scatter of +/- 1 magnitude
results in a factor of 1.6
uncertainty in distance