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The Formation and
Structure of Stars
Chapter 9
The Interstellar Medium (ISM)
•Gas: ~75% H, 25% He, traces of “metals”
•1% “dust” (silicates, carbon, heavy elements coated with ice,
About the size of the particles in smoke)
•150 m average distance between dust grains
•“Dense” => ~10 to 1000 atoms/cm3
•“Thin” ~ 0.1 atoms/cm3
Structure of the ISM
• HI clouds:
• Hot intercloud medium:
The ISM occurs mainly in two 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.
3 types of nebula
1. Emission
2. Reflection
3. Dark
Q: Why do emission
nebula look red and
reflection nebula blue?
We see absorption in elements
where the background stars are
too hot to form these lines
Narrow width (low temperature;
low density)
Multiple components (several
clouds of ISM with different
radial velocities)
=> Comes from the ISM
Evidence for the ISM
Interstellar reddening
Q: Why do
astronomers
rely heavily on
IR
observations?
Q: How do we know the ISM exists?
The Various Components of the
Interstellar Medium
Infrared observations reveal the
presence of cool, dusty gas.
X-ray observations reveal the
presence of hot gas.
Stellar formation from the ISM:
Must be triggered by
high mass stars –
• Give off intense
radiation
• Explode as SNs
Collapsing cloud
can form 10 to
1000 stars
• Association
• Cluster
star formation lecture powerpoint presentation
The Contraction of a Protostar
Q: Why do you think there’s a lower limit on the mass of a main-seq.
star?
The Contraction of a Protostar
Sun: ~30 million years
15 M: 160,000 years
0.2 M: 1 billion years
From Protostars to Stars
Ignition of H
 He
fusion
processes
Star emerges
from the
enshrouding
dust cocoon
Protostellar Disks and Jets – Herbig-Haro Objects
Herbig-Haro Object HH34
Q: What are the bipolar flows evidence of?
Globules
Bok globules:
~ 10 – 1000
solar masses;
Contracting to
form protostars
Evaporating gaseous globules
(“EGGs”): Newly forming stars
exposed by the ionizing radiation
from nearby massive stars
Observations of star formation:
200 solar mass star
star formation lecture powerpoint presentation
star formation lecture powerpoint presentation
star formation lecture powerpoint presentation
N 11B
Trifid
V838 Mon
Tarantula
N 49
star formation lecture powerpoint presentation
The Source of Stellar Energy
Stars produce energy by nuclear fusion of
hydrogen into helium.
In the sun, this
happens
primarily
through the
proton-proton
(P-P) chain
Q: How does the sun fuse H to He?
The CNO Cycle
Happens in stars
> 1.1 M
More efficient that
the P-P chain.
Requires high T
(>16 million K)
Q: Why does the
CNO require a
higher temp.
than the P-P
chain?
Fusion into Heavier Elements
Fusion into elements
heavier than C, O:
requires high
temperatures (>600
million K);
occurs only in very
massive stars (more
than 8 solar masses).
Stellar structure
Conservation of mass:
Weight of each shell = total weight
Conservation of energy:
E(out) = E(from within)
Hydrostatic equilibrium:
Pressure balances gravity
Energy transport:
Describes flow of energy
2
4
dM
r
dr
 

2
4
dL
r e
dr
 

2
dP GM
dr r

 
3 2
3
16
dT L
dr ac T r


 
Hydrostatic Equilibrium
Imagine 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 (II)
Outward pressure force must
exactly balance the weight of
all layers above, everywhere
in the star.
This is why we find stable stars on
such a narrow strip (main sequence)
in the Hertzsprung-Russell diagram.
Pressure-temperature thermostat
Q: How does the P-T thermostat control
the reactions in stars?
Energy Transport
Energy 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
Basically the same
structure for all stars
close to 1 solar mass.
Q: Why is convection in
stars important?
star formation lecture powerpoint presentation
Stellar Models
The 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.
…why stars initially all line up along the main sequence, and
why there’s a mass-luminosity relation….
The Life of Main-Sequence Stars
Stars gradually
exhaust their
hydrogen fuel.
They gradually
becoming brighter,
evolving off the
zero-age main
sequence (ZAMS).
3.5 2.5
fuel 1
rate of consumption
M
M M
   
Lifetime of a main-sequence
star (90% of total life is on
main-seq.)
The Lifetimes of Stars
on the Main Sequence
star formation lecture powerpoint presentation
star formation lecture powerpoint presentation
The Orion Nebula:
An Active Star-Forming Region
The Trapezium
The Orion Nebula
Infrared image: ~ 50
very young, cool, low-
mass stars
X-ray image: ~ 1000
very young, hot stars
less than 2
million years old
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
Protostars with protoplanetary disks
B3
B1
B1
O6
IR + visual
IR
Gas blown
away from
protostars

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star formation lecture powerpoint presentation

  • 1. The Formation and Structure of Stars Chapter 9
  • 2. The Interstellar Medium (ISM) •Gas: ~75% H, 25% He, traces of “metals” •1% “dust” (silicates, carbon, heavy elements coated with ice, About the size of the particles in smoke) •150 m average distance between dust grains •“Dense” => ~10 to 1000 atoms/cm3 •“Thin” ~ 0.1 atoms/cm3
  • 3. Structure of the ISM • HI clouds: • Hot intercloud medium: The ISM occurs mainly in two 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.
  • 4. 3 types of nebula 1. Emission 2. Reflection 3. Dark Q: Why do emission nebula look red and reflection nebula blue?
  • 5. We see absorption in elements where the background stars are too hot to form these lines Narrow width (low temperature; low density) Multiple components (several clouds of ISM with different radial velocities) => Comes from the ISM Evidence for the ISM
  • 6. Interstellar reddening Q: Why do astronomers rely heavily on IR observations?
  • 7. Q: How do we know the ISM exists?
  • 8. The Various Components of the Interstellar Medium Infrared observations reveal the presence of cool, dusty gas. X-ray observations reveal the presence of hot gas.
  • 9. Stellar formation from the ISM: Must be triggered by high mass stars – • Give off intense radiation • Explode as SNs Collapsing cloud can form 10 to 1000 stars • Association • Cluster
  • 11. The Contraction of a Protostar Q: Why do you think there’s a lower limit on the mass of a main-seq. star?
  • 12. The Contraction of a Protostar Sun: ~30 million years 15 M: 160,000 years 0.2 M: 1 billion years
  • 13. From Protostars to Stars Ignition of H  He fusion processes Star emerges from the enshrouding dust cocoon
  • 14. Protostellar Disks and Jets – Herbig-Haro Objects Herbig-Haro Object HH34 Q: What are the bipolar flows evidence of?
  • 15. Globules Bok globules: ~ 10 – 1000 solar masses; Contracting to form protostars
  • 16. Evaporating gaseous globules (“EGGs”): Newly forming stars exposed by the ionizing radiation from nearby massive stars Observations of star formation:
  • 21. N 11B
  • 25. The Source of Stellar Energy Stars produce energy by nuclear fusion of hydrogen into helium. In the sun, this happens primarily through the proton-proton (P-P) chain Q: How does the sun fuse H to He?
  • 26. The CNO Cycle Happens in stars > 1.1 M More efficient that the P-P chain. Requires high T (>16 million K) Q: Why does the CNO require a higher temp. than the P-P chain?
  • 27. Fusion into Heavier Elements Fusion into elements heavier than C, O: requires high temperatures (>600 million K); occurs only in very massive stars (more than 8 solar masses).
  • 28. Stellar structure Conservation of mass: Weight of each shell = total weight Conservation of energy: E(out) = E(from within) Hydrostatic equilibrium: Pressure balances gravity Energy transport: Describes flow of energy 2 4 dM r dr    2 4 dL r e dr    2 dP GM dr r    3 2 3 16 dT L dr ac T r    
  • 29. Hydrostatic Equilibrium Imagine 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
  • 30. Hydrostatic Equilibrium (II) Outward pressure force must exactly balance the weight of all layers above, everywhere in the star. This is why we find stable stars on such a narrow strip (main sequence) in the Hertzsprung-Russell diagram. Pressure-temperature thermostat Q: How does the P-T thermostat control the reactions in stars?
  • 31. Energy Transport Energy 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 Basically the same structure for all stars close to 1 solar mass. Q: Why is convection in stars important?
  • 33. Stellar Models The 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. …why stars initially all line up along the main sequence, and why there’s a mass-luminosity relation….
  • 34. The Life of Main-Sequence Stars Stars gradually exhaust their hydrogen fuel. They gradually becoming brighter, evolving off the zero-age main sequence (ZAMS). 3.5 2.5 fuel 1 rate of consumption M M M     Lifetime of a main-sequence star (90% of total life is on main-seq.)
  • 35. The Lifetimes of Stars on the Main Sequence
  • 38. The Orion Nebula: An Active Star-Forming Region
  • 39. The Trapezium The Orion Nebula Infrared image: ~ 50 very young, cool, low- mass stars X-ray image: ~ 1000 very young, hot stars less than 2 million years old
  • 40. 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 Protostars with protoplanetary disks B3 B1 B1 O6 IR + visual IR Gas blown away from protostars