Lecture 13 - The Interstellar Medium (2/25/99)
 Stellar Structure II --- | --- 
Star Formation
Stellar Structure II --- | --- 
Star Formation
 
 Reading:
Reading: 
Chapter 11-4, 15-1, 15-2 (ZG4) 
 Notes: 
pages 51 - 54
M42, the Great Nebula in Orion, a site of ongoing massive star 
formation.
 (Courtesy 
Bill Arnett/Jason Ware)
|  | Key Question: | What are the dark nebulae made of? | 
|---|
|  | Key Principle: | The 21-cm HI line | 
|---|
|  | Key Problem: | Mass-Luminosity Relation | 
|---|
Investigations:
- Interstellar Dust
- What does interstellar dust do to starlight?
    
- Why is reflected light blue, and transmitted light reddened?
    
- How is dust extinction related to optical depth?
    
- What is the typical size of dust grains?
    
- What does A_v = 1 mag of extinction imply for optical depth?
    
- What is the typical visual extinction in mag per kpc in the galactic
        plane?
    
- What is the color excess in B-V corresponding to 1 mag A_v?
    
- What is the reddening vector in the H-R diagram?
    
- What effect does extinction have on Cepheid distances?
    
- What effect does extinction have on star counts?
    
- What sort of chemical reactions can take place on dust grains?
    
- What is the interstellar medium (ISM) and what is it 
        composed of?
    
 
- H II Regions
- Why do hot O and B stars ionize the gas around them?
    
- What is an H II region?
    
- What wavelengths are relevant for ionizing photons to
        make an H II region? (For O9 star, n_ion ~ 10^49/s)
    
- How does equilibrium between ionization and recombination
        determine the size of an H II region?
    
- What is a Stromgren sphere?
    
- Why do we need only consider recombination to levels n > 1 above
        the ground state? (a2 ~ 10^-19 m^3/s)
    
- What is the typical size for an H II region at T = 8000 K with
        n_H ~ 10^3/m^3 and n_e ~ 10^9/m^3
    
 
- Atomic and Molecular Lines in the ISM
- Using the Boltzmann equation, what energy level do you expect the
        atoms to be in for a cold cloud with T < 100 K?  Do you expect strong
        Balmer lines, for example?
    
- What is a hyperfine transition?
    
- Why are there two spin states for neutral hydrogen?
    
- What is the energy difference corresponding to the 21-cm line
        at 1.420406 GHz?
    
- How does H I emission in the 21-cm line allow us to map the gas
        in the galaxy?
    
- What are the vibrational and rotational transitions
        in molecules?
    
- How do molecular lines allow us to probe the compositions of cold
        molecular clouds?
    
- How many species of molecules have been discovered in the ISM?
    
- What is the most complex molecule seen?
    
- How do the rotational level populations for a transition at frequency
        v (eg. CO 1-0 at v=118 GHz) follow the Boltzmann distribution?
    
- Why is CO an important tracer in the ISM?
    
 
The Interstellar Medium in Outline
- Gravitational Collapse
- Gravity is always attracting, there is no "anti-gravity" repulsion.
    
- What do you think happens if you start with a bunch of matter
	(of any type) distributed far across space, and let gravity do
	its work?
    
- Unless you make the matter distribution exactly uniform and infinite
	then it will always collapse eventually, unless something 
	stops it.
    
- What can stop gravitational collapse?
    
- The matter can hit something first, namely the rest of the matter
	that is falling in also.  These collisions cause heat and pressure
	which resists the collapse.  This is called gas pressure.
    
- If the collapsing cloud of matter becomes hot enough, and starts
	emitting photons like stars do, then the light pressure can stop
	the collapse.  This is called radiation pressure.
    
- Some other sort of pressure, like that from magnetic fields, can
	stop the collapse.  This is called magnetic pressure.
    
- We know our solar system is stable and not collapsing, but the
	planets are orbiting.  They possess momentum, specifically, 
	angular momentum that keeps it spinning instead of 
	collapsing.
    
- It turns out that stars (and gas giant planets like Jupiter and
	Saturn) use gas and radiation pressure to support themselves against
	gravity.  This is what defines the size of a star.
    
- It also turns out that in the early stages of star formation, when
	large gas clouds have to collapse by many orders of magnitude in
	size to form stars, that magnetic pressure (and to some extent
	gas pressure) and angular momentum must be overcome.
    
- We will discuss the star formation process in more detail
	in the next lecture.
    
- For now, where is the stuff from which stars are made?
    
 
- A View of the Interstellar Medium
- Early in the history of telescopic astronomy, it was noticed 
	that in addition to lots and lots of stars, there appeared to
	be fuzzy patches, or clouds, in the celestial sky.
    
- These were called nebulae, or nebula in the singular,
	which is Latin for "cloud".
    
- Catalogs for nebulae were made so that people would not confuse them
	with fuzzy comets, which they were more interested in.
    
- What are the nebulae? What different kinds do we see?  This is
        the usual first step in observational science - classify the
	objects that we find!
    
- Diffuse Nebulae - amorphous bright fuzzy blobs, sometimes
	with one or more bright stars in the center.  These turn out to
        be gas clouds ionized and lit up by very bright young stars.
    
- Planetary Nebulae - shells or rings of bright nebulosity 
        surrounding a more or less hollow center.  These turn out to be 
        shells of matter thrown off of a dying star.
    
- Supernova Remnant - veil like wisps, filamentary rings,
        or a filled shell with lots of tendrils (often similar in appearance
        to diffuse nebulae).  These turn out to be the result of titanic
        stellar explosions (supernovae) marking the death of a massive star.
    
- Dark Nebulae - dark clouds that block out the stars behind
        them, and redden those few stars that manage to be seen through them.
        Often look like "holes" or "gaps" in the Milky Way.  These are 
        relatively dense clouds of gas containing dust grains that absorb 
        visible light.  Some times dark nebulae are seen in conjunction with
        bright diffuse nebulae, which seem to live on the edges of dark
        clouds.
    
- Diffuse nebulae can shine by their own light if they are hot,
        then being called emission nebulae.  Lines of hydrogen,
        carbon, oxygen, calcium, and other atoms can be seen their 
        spectrum.  Most bright diffuse nebulae are emission nebulae.
    
- Some diffuse nebulae shine by reflected starlight, and are thus
        called reflection nebulae.  Faint blue wisps around the
        stars of the Pleiades, a star cluster in the constellation Taurus
        visible to the naked eye are a refection nebulae caused by the
        bright stars.
    
- The nebulae that we are interested in for star formation are the
        dark nebulae, which contain large amounts of cold gas primed for
        gravitational collapse and the birthing of stars!
    
 
- What is the Interstellar Medium Made Of?
- We call all this gas and nebulosity the interstellar medium,
        the stuff "between the stars", like interstate means between states.
        We abbreviate interstellar medium as ISM.
    
- From spectra of the nebulae, we know they are made of gas, just like
        the photospheres of stars like our Sun.
    
- The gas in the emission nebulae often have compositions very similar
        to the Sun's: mostly hydrogen and helium, with traces of other elements
        like carbon, nitrogen, oxygen, and iron.  In fact, it is as if they
        came from stars (...hmmmmm...).
    
- There is also dust in the ISM, small grains about 1 micron
        (10^-6 m) in size.  About 1% of the ISM is in dust grains.
    
- Scattering of light off of dust grains is what reddens the light
        of stars seen through dust clouds.  The short wavelength blue photons
	are more easily scattered than the longer wavelength red photons.
        This same effect reddens the Sun at sunset - and after dust storms
        or volcano eruptions or big fires sunsets are spectacularly red.
    
- The dust is made of solids, like ice, carbon compounds, silicates,
        and iron.
    
- Dust is formed in low temperature regions, below 100K or so,
        since high temperatures will cause collisions and sputtering
        of the grains thus destroying them.
    
- The surfaces of dust grains can act as a matrix to hold molecules
        close together and allow chemistry to occur.  Some very large
        molecules have been detected in space, with more than ten atoms.
        These tend to be chains of hydrocarbons and other organic molecules,
        and there are claims of seeing some proteins, like those that make
        up DNA, in some molecular clouds!  These complex molecules are 
        believed to be made on the surfaces of grains.  In the past decade,
        the field of cosmochemistry has grown to study the formation
        of these molecules.
    
- The densities in the molecular clouds are as high as 10^5 atoms/cm^3.
        This is still very tenouous, these dark clouds are still better 
        vacuums than anything we can make here on Earth!
    
- Molecular clouds range in masses from 100 up to 10^8 solar masses!
        You can make lots of stars out of that much stuff.
    
 
- Atomic Hydrogen Clouds
- Neutral hydrogen atoms (ionization state H I) make up about
        22% of the interstellar medium.
    
- These clouds range in density and temperature from 3000K at
        0.3 atoms/cm^3 for warm clouds to 100K at 50 atoms/cm^3 for
        cold clouds.
    
- The primary way of identifying clouds of H I is through the
        21 cm line.
    
- The hydrogen line at a wavelength of 21cm in the radio spectrum
        is caused by a slight energy difference between states of the
        hydrogen atom where the proton and electron spins are aligned
        or opposite.
    
- If you remember our discussion of the 
        hydrogen energy levels and quantum numbers, then you will remember
        that particles like electrons and protons have a property called
        spin (quantum number s = +/- 1/2) which is analogous
        to picturing the particle as a little spinning top.
    
- Because the proton and electron are electrically charged, the spin
        means that they act as little magnets.  Because they are charged
        oppositely, their magnetic poles are aligned oppositely with respect
        to the spin in the electron versus the proton (if their spins are
        aligned, then their magnetic poles are opposite).
    
- If you've played with magnets, then you know that they like to
        be oriented oppositely - the opposite poles attract and the 
        like poles repel.
    
- Thus, if the spins of the proton and electron in the hydrogen atom
        are aligned (poles opposite), then there is a tiny extra attraction
        which is like decreasing the energy of the ground
        state level (making the electron slightly more bound).
    
- If the spins of the proton and elecron are opposing (poles aligned)
        there is a tiny repulsion, which is like increasing the energy of
        the ground state level.
    
- The energy difference between these two configurations of the ground
        state is tiny: the photon wavelength to excite this transition is
        21cm, compared to 121.6 nm for the transition from the ground state
        to the next higher electron level.  Q: How many times smaller
        is this energy difference?  What is this difference in electron volts
        (eV)?
    
- If a photon of wavelength 21cm is absorbed or emitted, the spins
        flip relative to each other.
    
- The emission (and absorption) of the 21 cm line by clouds of hydrogen
        can be observed with large radio telescopes.  The line was predicted
        by the Dutch astrophysicist van der Hulst in 1945, and first observed
        by Ewen and Purcell of Harvard in 1951.
    
- The 21 cm emission has been used to map out the H I clouds in our
        galaxy, and to detect H I in other galaxies.
    
 
- Molecular Clouds
- If a cloud is cold enough, then the atoms have the chance to
        come together and form molecules.  This is able to happen in
        clouds with temperatures of roughly 100K or less.
    
- These clouds tend to be buried deep within atomic H I clouds.
    
- These are the coldest (10K - 100K) and densest (10^4 - 10^5 atoms/cm^3)
        clouds.
    
- These clouds are made up mostly of molecular hydrogen (H2), which is
        two atoms of hydrogen bound together.  The dissociation energy
        for H2, the energy needed to break apart the molecule, is 4.48 eV.
    
- Carbon monoxide CO is also seen in clouds.  CO has a dissociation 
        energy of 9.6 eV, and it thus hardier than H2.
    
- There are many other diatomic (two-atom) molecules found in 
        molecular clouds, such as C2, CO, CN, CH, CS, SO, SiO, OH, etc.
    
- More complex molecules like H2O (water!), HCN (cyanide!), H2S, 
        as well as alcohols and molecules with more than 13 atoms have
        also been seen in these clouds!  As of the end of 1993, over
        93 different molecules have been seen in the ISM.  That number
        has increased in the years since then.
    
- The presence of these molecules has been identified by observing
        molecular lines, which like the atomic lines like the
        Balmer series of hydrogen, correspond to energy levels in the
        molecule.
    
- The molecular energy levels correspond not to electron orbits like
        in atoms, but to vibrations and rotations of the molecule.
    
- Vibrational lines are the most energetic, with typical 
        wavelengths of 0.1 mm or shorter.  For H2, the series limit is 
        4.48 eV (277 nm), with the "alpha" transition at 2275 nm, or
        2.275 microns, in the far-infrared.  The CO "alpha" vibrational 
        transition is at 4.6 microns.
    
- Rotational Lines are lower in energy, and thus come out in
        in the millimeter wave range.  It turns out that to get a rotational 
        transition, you need two (or more) atoms of different mass in the
        molecule - H2 has no rotational transitions, because it is symmetric!
        The "alpha" rotational transition for CO is at 2.7 mm, this is one
        of the primary lines used to map out molecular clouds.
    
- Because the molecular clouds are the coldest and densest of the
        gas clouds, they are the places where stars are formed.  They
        are in many ways "stellar nurseries".
    
 
- The Orion Molecular Cloud
- One of the most spectacular and nearest large molecular clouds
        is the Orion Molecular Cloud, which covers much of the
        constellation of Orion, and contains the bright diffuse Orion
        Nebula.
    
- The cloud is at a distance of 460 pc from us, and extends over
        30pc in size.  The total mass of molecular gas in the cloud
        is around 2 x 10^5 times the mass of the Sun.
    
- The oldest stars formed out of the cloud are near the shoulder
        of Orion, and are around 12 million years old.  The youngest
        stars that we see are in the center of the Orion Nebula itself,
        and are about 2 million years old.  The sun is about 4.5 billion
        years old in comparison.
    
- Star formation in Orion uses less than 25% of the gas in any given
        region, there rest is blown away.
    
- Because there seems to be a pattern to the ages, with the oldest
        stars farthest away from the nebula, we believe that there is
        progressive star formation where the formation of the first
        stars triggers the next stars to form.  Thus, star formation sweeps
        through the cloud like a forest fire!
    
- Note that the Sun itself was not formed with the first stars, its 
        formation was triggered later on!  In fact, basically all of the
        elements heavier than helium were formed in stars, then blown out
        in supernovae.  Our bodies are made up of stuff that was cooked in
        long dead stars!
    
 
 
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Steven T. Myers