Act One
(The setting: A vast cloud of molecular hydrogen gas (H2) and some dust.
Enter some compressive disturbance and the cloud begins to collapse.)
Scene One: The Initial Collapse
- Something triggers the collapse of a huge nebula. The nebula measures
many
light years across and contains several thousand solar masses of material.
Average densities are on the order of 10^3 particles/cc and typical temperatures
are a "chilly" 10 K - 50 K!
-
gravitational potential energy is released - heats up the cloud. This turns
out to be a trick that a star will use many times during its life.
-
material piles up at the cloud center, density rises in the center.
-
the core begins to collapse faster than the outer envelope.
Scene Two: Fragmentation and Further Collapse
- After several million years the
collapsing cloud begins to fragment into
numerous smaller clouds that each continue to collapse. The following descriptions
apply to each of these perhaps thousands of "cloudlets".
-
the increasing frequency of collisions between H2 molecules is the equivalent
of heating up the cloud. The dust grains also heat up and begin to re-radiate
this energy in the Infrared region.
-
the core is warmed up to several hundred degrees K, the collapse slows
down dramatically. Densities are now approaching 10^6 particles/cc and
the cloud is about 100 times the size of our solar system.
Scene Three - It's Heating Up!
-
material from the envelope continues to rain onto the core causing it to
collapse slowly under the added weight.
-
the core continues to heat.
- the contracting cloud is also
spinning. In order to conserve angular momentum
(the "figure skater effect") the spin rate increases and the cloud flattens
out into a disk. Rapid spinning begins to inhibit collapse.
- the magnetic field of the collapsing
cloud becomes more concentrated as
the cloud collapses and begins to "stiffen" - pushing back and further
inhibiting collapse.
-
when the core reaches 2000 K the H2 molecules break apart. This takes a
lot of energy - in order to pay the bill - the core collapses again. Eventually
the core reaches approximately 10 000 K and the cloud begins to resemble
a star. At about 30 times the size of our Sun the cloud has become a Protostar.
Scene Four: A STAR IS BORN!
-
the core collapses from a diameter of about 4 AU to the size of the sun,
heats up considerably and becomes hot enough for nuclear fusion to begin.
-
the outer envelope - like a womb - shields the entire event from view at
optical wavelengths. The dust in the envelope heats up and becomes a very
large region glowing brightly in the infrared part of the spectrum.
- the outer envelope is blown away
and a pre-main sequence star emerges.
This is a violent process - a rapidly spinning and still collapsing outer
disk collides with a now expanding shell from the newly formed star. Motion
above and below the rotational plane of the nebula is easier and hence
material "squirts" away at right angles to the disk.
Act Two - Scene One
(The setting: Astronomers from
around the world are using an "armada" of
telescopes to study star birth)
Scene One: The IR-View
-
An astronomer adjusts the Infrared detector on her telescope and directs
to the Serpens star forming region. An intense knot of IR radiation bursts
through.
Scene Two: "Hubble-Vision"
-
Researchers using the HST are producing exquisite images of star formation.
Some of these images support the basic ideas sketched in the previous passages
while others are extending our understanding in surprising and un-anticipated
ways. The images show clearly the jet like structures (bi-polar flows)
ejected from the collapsing stellar cloud and protostar.
- Associated with jets are bright
knots of light called Herbig-Haro objects.
We think that these are the result of shock-wave heating produced by supersonic
matter ejected along the jets. As this matter plows into dust and gas left
over from the collapsing nebula it heats the gas and produces these bright,
fast moving "blobs".
-
Another fascinating set of images are those taken in the heart of the Orion
Nebula. Small condensations called proplyds are thought to be actual images
of protostars surrounded by their accretion disks.
Scene Four: An Orion Nebula Spectacular:
A November 20, 1995 release of Hubble images of M42 provides stunning confirmation
of many of the ideas presented here. Follow these links and hang on!
Scene Five: Radio Tracers
- A colleague in West Germany monitors "bright" microwave emissions from
the same area. This is clear evidence - a star has recently formed. Furthermore,
observations of tracer molecules like formaldehyde or carbon monoxide give
evidence that regions in this "stellar" nursery continue to collapse.
Act Three - Scene One
(The setting: An astronomer is lecturing to his first year class. They
are having trouble paying attention until he shows them an HR plot. Instantly
they realize the import of what he is telling them (they are very bright).)
The HR diagram IS ALIVE! The salient features on the HR diagram are numbered
along the HYASHI track or path that the star's changing appearance produces:
- the protostar now has a photosphere but has not yet achieved core temperatures
high enough to fuse hydrogen. At this stage the star has a radius about 30
times that of our Sun. It is cool but its enormous size allows it to shine
very brightly. We will probably not get a good view, however, because gas
and dust shroud the protostar.
- the star continues to collapse and heat. It will also be spinning rapidly
and possibly ejecting matter. The star may enter what is called the T-Tauri
phase for a short period. The shrinking size will reduce the luminosity of
the star.
- Core contraction has finally produced high enough temperatures and collision
rates to support thermonuclear reactions in the core. The star settles onto
the main sequence where it will spend about 90% of its life.
The entire process - from large cloud
to sun-like star takes about 30 million
years. This is just the beginning of a discussion of stellar evolution
- how a star "grows up", that will continue to the end of the term.
Seeds:
Chp11, all
Kaufmann: Chp 20; pgs 364-383
