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The space between the stars is not completely empty, but filled with very
dilute gas and dust, producing some of the most beautiful objects in the sky.
We are interested in the interstellar medium because:
a) Dense interstellar clouds are the birth place of stars.
b) Dark clouds alter and absorb the light from stars behind them.
The Interstellar Medium (ISM)
Three kinds of nebulae1) Emission Nebulae (HII Regions)
A hot star illuminates a gas cloud;
excites and/or ionizes the gas
(electrons kicked into
higher energy states);
electrons recombining, falling back to ground state
produce emission lines The Fox Fur Nebula NGC 2246The Trifid Nebula
2) Reflection Nebulae
Star illuminates gas and dust cloud
star light is reflected by the dust
reflection nebula appears blue because blue light is scattered by larger angles than
red light
same phenomenon makes the day sky
appear blue (if it’s not cloudy)
3) Dark Nebulae
Barnard 86
Dense clouds of gas and dust absorb the light from the stars behind;
appear dark in front of
the brighter background
Horsehead Nebula
Interstellar Reddening
Visible Infrared
Barnard 68
Blue light is strongly scattered and absorbed
by interstellar clouds.
Red light can more easily penetrate the cloud, but
it is still absorbed to some extent.
Infrared radiation is
hardly absorbed at
all.
Interstellar clouds make background stars appear
redder.
Interstellar Absorption LinesThe interstellar medium produces
absorption lines in the spectra of stars. These can be
distinguished from stellar absorption
lines through:
a) Absorption from wrong ionization states Narrow absorption lines from Ca II: Too low
ionization state and too narrow for the O star in the background; multiple componentsb) Small line width
(too low temperature; too low density)
c) Multiple components
(several clouds of ISM with different radial velocities)
Structure of the ISM
• HI clouds:
• Hot intercloud medium:
The ISM occurs in two main types of clouds:
Cold (T ~ 100 K) clouds of neutral hydrogen (HI);
moderate density (n ~ 10 – a few hundred atoms/cm3);
size: ~ 100 pc
Hot (T ~ a few 1000 K), ionized hydrogen (HII);
low density (n ~ 0.1 atom/cm3);
gas can remain ionized because of very low density
Shocks Triggering Star Formation
The gas in the ISM needs to be compressed in order to collapse and form stars: Shocks traveling
through interstellar space can do this.
From Protostars to Stars
Ignition of H → He fusion processes
Star emerges from the
enshrouding dust cocoon
Evidence of Star FormationNebula around S Monocerotis:
Contains many massive, very young stars,
including T Tauri Stars: strongly variable; bright
in the infrared.
Protostellar Disks and Jets – Herbig Haro Objects
Disks of matter accreted onto the protostar (“accretion disks”) often lead to the formation of jets (directed outflows; bipolar outflows): Herbig Haro Objects
GlobulesEvaporating Gaseous
Globules (“EGGs”): Newly forming stars exposed by the ionizing radiation from
nearby massive stars.
Winds from Hot StarsVery young, hot stars produce massive stellar winds,
blowing parts of it away into interstellar space.
Eta Carinae
The Trapezium
The Orion Nebula
The 4 trapezium stars: Brightest, very young
(less than 2 million years old) stars in the central region of the
Orion nebula
Infrared image: ~ 50 very young, cool, low-
mass starsX-ray image: ~ 1000 very young, hot stars
Only one of the trapezium stars is hot
enough to ionize hydrogen in the Orion
nebula.
The Becklin-Neugebauer Object (BN): Hot star, just reaching the main
sequence
Kleinmann-Low nebula (KL): Cluster
of cool, young protostars detectable only in the
infrared
Spectral types of the trapezium
stars
Visual image of the Orion NebulaProtostars with protoplanetary disks
B3
B1
B1
O6
The Source of Stellar EnergyRecall from our discussion of the sun:
Stars produce energy by nuclear fusion of hydrogen into helium
In the sun, this happens primarily
through the proton-proton (PP) chain.
The CNO Cycle
In stars slightly more massive than the sun, a more powerful
energy generation mechanism than
the PP chain takes over.
The CNO Cycle
Fusion into Heavier Elements
Fusion into heavier elements than C, O:
requires very high temperatures; occurs only in very massive stars (more than 8
solar masses)
Hydrostatic EquilibriumImagine a star’s interior composed of individual
shells.
Within each shell, two forces have to be in
equilibrium with each other:
Outward pressure from the interior
Gravity, i.e. the weight from all layers above
Hydrostatic Equilibrium
Outward pressure force must exactly balance the
weight of all layers above everywhere in
the star.
This condition uniquely determines the interior structure of the star.
This is why we find stable stars on such a narrow strip
(Main Sequence) in the Hertzsprung-Russell diagram.
Energy TransportEnergy generated in the star’s center must be
transported to the surface.
Inner layers of the sun:
Radiative energy transport
Outer layers of the sun
(including photosphere):
Convection
Stellar Structure
Temperature, density and pressure decreasing
Energy generation via nuclear fusion
Energy transport via radiation
Energy transport via convection
Flo
w o
f en
erg
y
Basically the same structure for all stars with approx. 1 solar
mass or less.
Sun
Stellar ModelsThe structure and evolution of a star is
determined by the laws of:• Hydrostatic equilibrium
• Energy transport
• Conservation of mass
• Conservation of energy
A star’s mass (and chemical composition) completely determines
its properties.
That’s why stars initially all line up along the main sequence.
Interactions of Stars and their Environment
Young, massive stars excite the remaining gas of their
star forming regions, forming HII regions.
Supernova explosions of the most massive stars inflate and blow
away remaining gas of star forming regions.
The Life of Main Sequence Stars
Stars gradually exhaust their
hydrogen fuel.
In this process of aging, they are
gradually becoming brighter,
evolving off the zero-age main
sequence.