Title: Stellar Astronomy
1Stellar Astronomy
- Paul J. Thomas
- Department of Physics and Astronomy
- UW - Eau Claire
2Astronomical Magnitudes
- Measures apparent brightness of objects.
- The brighter the object, the smaller (or more
negative) the magnitude. - Each magnitude is 2.512 brighter than the next
lowest step. - 100 6 mag. stars 1 1 mag. star.
- 1011 28 mag. stars 1 1 mag. star.
3Examples of Magnitudes
- Sun -26.5
- Full Moon -12
- Venus (maximum) -4
- Sirius -1.5
- Naked eye limit 6
- Binocular limit 10
- 5 m telescope 25
- HST 28
4Intrinsic vs. Apparent Brightness
- Intrinsic brightness is the measurement of how
luminous a star actually is. - Apparent brightness is the measurement of how
luminous a star appears to be. It is affected by
the distance to a star. - We use magnitudes to measure the brightness of a
star.
5Intrinsic Brightness
- The intrinsic brightness of a star is given by
- Absolute magnitude (M) the magnitude a star
would have at a distance of 10 parsecs (32.6
light years) - Luminosity (L?) brightness compared to the Sun.
6Intrinsic vs. Apparent Brightness
Vega
Altair
Deneb
Vega and Deneb are similar in apparent
brightness But Deneb is over 100 further
away! So Deneb must have a greater intrinsic
brightness!
7Intrinsic vs. Apparent Brightness
- Vega
- m 0.04
- M 0.5
- L 54 L?
- r 26.5 ly
- Deneb
- m 1.26
- M -7.1
- L 59,000 L?
- r 3000 ly
8Spectral Sequence
- O 28,000 K
- B 10,000 - 28,000 K
- A 7,500 - 10,000 K
- F 6,000 - 7,500 K
- G 5,000 - 6,000 K
- K 3,500 - 5,000 K
- M, R, N, S
9Spectral Sequence
- OBAFGKMRNS
- Oh, be a fine girl/guy kiss me, right now -
smack!
10Sizes of stars
- Using parallax, we can determine the intrinsic
brightness of stars. - Stars that are hot and intrinsically dim are
small (e.g. white dwarfs). - Stars that are cool and intrinsically bright are
large (e.g. red giants).
11The Hertzsprung-Russell Diagram
- Developed in 1912 by Ejnar Hertzsprung (Denmark)
and Henry Norris Russell (USA). - A statistical plot of luminosity vs. surface
temperature for many stars.
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14A Variety of Main Sequence Stars
- Temperature
- Hottest 50,000 K
- Sun 5,800 K
- Coldest 2,500 K
15A Variety of Main Sequence Stars
- Luminosity
- Most Luminous 800,000 L? (M -9.9)
- Sun 1 L? (M 4.8)
- Least Luminous 10-6 L? (M 20)
16A Variety of Main Sequence Stars
- Radius
- Biggest 20 R?
- Sun 1 R?
- Smallest 0.1 R?
17Determining the Mass of Stars
- 50 of all stars are in a binary system (2 or
more stars orbiting around each other). - By observing their separation and their period,
we can determine their combined mass by Keplers
Third Law
18A Variety of Main Sequence Stars
- Mass
- Most massive 60 M?
- Sun 1 M?
- Least massive 0.06 M?
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20How does a star shine?
- Stars are balls of hot gas. They support
themselves against gravity by the expansion of
gas in their interiors.
21How does a star shine?
- The centers of stars must very hot. (The center
of the Sun is about 15,000,000 K). - At these temperatures, hydrogen can be converted
to helium by nuclear fusion.
22Nuclear Fusion pp chain
- Mass of 4 protons 2 electrons
- 6.694 10-24 g
- Mass of 4He nucleus
- 6.644 10-24 g
- Difference 0.050 10-24 g
- Energy released (E mc2) 4.4 10-12 J
- 6 1014 g of H ? He per second!
23Energy from Nuclear Fusion
- 4.4 ? 10-12 J for each He nucleus produced
- (there are 1.5 ? 1023 He nuclei per g)
- 6.62 ? 1011 J for each g of He produced
- (6 ? 1014 g of He is produced every second)
- 3.97 ? 1026 W of power
24Stellar Evolution
- Stars form as groups in bright nebulae, e.g. the
Orion Nebula. - The mass of a star determines its evolution.
- The more massive a star, the shorter its Main
Sequence lifetime. - Stars generate energy by burning light elements
to heavy elements nucleosynthesis.
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26Life of a 0.1 M? Star
- We dont know much about these brown dwarfs.
- They are hard to see, and might be present in our
galaxy in large numbers. - MS lifetime probably 100 billion years.
27HST Views a Brown Dwarf
28Life of a 1.0 M? Star
- MS lifetime 1010 y.
- Burns H ? He in core on MS.
- Then becomes Red Giant and burns H ? He in shell.
- Starts to burn He ? C in core (helium flash).
- Becomes variable star.
- Final stage C white dwarf surrounded by
planetary nebula.
29A 1.0 M? Star
30Planetary Nebula
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32White Dwarfs
- R 7000 km, T 30,000 K.
- M
- ? 107 g/cm3.
- Composed of electron degenerate material.
33White Dwarfs
34Life of a 25 M? Star
- MS lifetime 7 My.
- Burns H ? He in core on MS.
- Then becomes Supergiant and burns He ? C, N, O ?
Ne ? Mg ? Fe in shells and core.
35A 25 M? Star, Part 1
36A 25 M? Star, Part 2
37Just before the Supernova
- Burning in concentric shells of increasing
nuclear mass. - Fusion of Fe absorbs energy, and core collapses,
triggering supernova. - Core becomes neutron star or black hole.
38Eta Carinae Future Supernova
39Luminosity of Supernovae
- M -20
- 5 ? 109 solar luminosity
- Period of maximum brightness 20 days
40Supernova 1987a
41Supernova 1987a
42The Crab Nebula, a SNR
43Neutron Stars
- R 20 km.
- M 1.4 M? - 3 M?.
- ? 3 1014 g/cm3.
- Composed of neutron degenerate material.
- In a neutron star, the electrons and protons have
been squeezed together, leaving only neutrons.
44Pulsars
- First discovered in 1967 by Jocelyn Bell. She
detected radio pulses with a period of 1.3373011
s. - We think they are very rapidly rotating neutron
stars. - They radiate pulses at all wavelengths.
45Pulsars
- Pulsars are rapidly rotating neutron stars.
- The magnetic field of the neutron star
accelerates charged particles in the SNR. - Pulses are produced by synchrotron radiation.
46Planets around Pulsars
- Alex Wolszczan and co-workers have discovered
three planets around pulsar PSR 125712.
47Black Holes
- Not even light can escape from a body if the
escape speed exceeds the speed of light.
48Black Hole Size
- The Schwarzschild Radius is the radius of a black
hole.
49Singularities and Event Horizons
- At the center of a black hole is a singularity a
point of infinite density and zero size. - We cant see this, as light cannot escape from
the region around it. This region is bounded by
the Event Horizon. The radius of the Event
Horizon is Rs.
50Einsteins Theory of General Relativity
- A new way of looking at gravity in the universe.
- The three dimensions of space and the dimension
of time form a surface of spacetime. - This surface is distorted by the presence of mass.
51Albert Einstein
- One thing I have learned in a long life that
all our science, measured against reality, is
primitive and childlike -- and yet it is the most
precious thing we have.
52Einsteins Theory of General Relativity
- Light moves in straight lines through spacetime,
and so is deflected by the presence of mass,
which distorts spacetime. This is gravitational
lensing. - Planets orbit around stars because they move in a
spacetime distortion. - This predicts the motions of planets better than
Newtons laws.
53Gravitational Lensing
54Gravitational Lensing
- British astronomers observed a total eclipse in
May 1919, from an island off West Africa and to
Brazil. They succeeded in
photographing stars near the eclipsed sun. The
starlight had been deflected just as Einstein had
predicted.
55Gravitational Lensing
- HST image of a cluster of galaxies. The
concentrated mass of the cluster warps space
around it, bending light from galaxies far beyond
the cluster. The images of these galaxies appears
as streaks and arcs in this image.
56General Relativity and Black Holes
- In General Relativity, a black hole is a tunnel
in spacetime. - An object falling into a black hole will appear
to be - greatly redshifted
- ageing more slowly.
- It will also be torn apart by tidal forces.
57Evidence for Black Holes
- X-ray binaries are stars where a normal star has
an unseen companion. X-rays are observed coming
from the system, probably from an accretion disk
surrounding the unseen companion. - The unseen companion is pulling material off the
normal star. It must be a collapsar.
58Cygnus X-1
- The optical companion, HDE 226868, is an O9.7
supergiant, with a mass 30 M?. - The total mass of the system is 37 M ?.
- The unseen companion has a mass 7 M?.
- This exceeds the stability limit for a neutron
star.
59Cygnus X-1
60Sagittarius A