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Gravity makes cloud want to collapse. Outward gas pressure resists collapse, like air in a bike pump. Star Formation. Stars form out of molecular gas clouds. Clouds must collapse to form stars (remember, stars are ~10 20 x denser than a molecular cloud).
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Gravity makes cloud want to collapse. Outward gas pressure resists collapse, like air in a bike pump. Star Formation Stars form out of molecular gas clouds. Clouds must collapse to form stars (remember, stars are ~1020 x denser than a molecular cloud). Probably new molecular clouds form continually out of less dense gas. Some collapse under their own gravity. Others may be more stable. Magnetic fields and rotation also have some influence.
When a cloud starts to collapse, it should fragment. Fragments then collapse on their own, fragmenting further. End product is 100’s or 1000’s of dense clumps each destined to form star, binary star, etc. Hence a cloud gives birth to a cluster of stars.
Fragments in Orion molecular cloud, about 1000 x denser than average gas in cloud.
As a clump collapses, it heats up. Becomes very luminous. Now a protostar. May form proto-planetary disk. DEMO Protostar and proto-planetary disk in Orion 1700 AU Eventually hot and dense enough => spectrum approximately black-body. Can place on HR diagram. Protostar follows “Hayashi tracks” Dramatic mass loss
Finally, fusion starts, stopping collapse: a star! Star reaches Main Sequence at end of Hayashi Track One cloud (103 - 106 MSun) forms many stars, mainly in clusters, in different parts at different times. Massive stars (50-100 MSun) take about 106 years to form, least massive (0.1 MSun) about 109 years. Lower mass stars more likely to form. In Milky Way, a few stars form every year.
Brown Dwarfs Some protostars not massive (< 0.08 MSun) enough to begin fusion. These are Brown Dwarfs or failed stars. Very difficult to detect because so faint. First seen in 1994 with Palomar 200”. How many are there?
The Eagle Nebula Molecular cloud surface illuminated by nearby hot stars. Radiation evaporates the surface, revealing a dense globule - a protostar. Other hot stars illuminating these clouds Shadow of the protostar protects a column of gas behind it. Eventually structure separates from the cloud, and the protostar will be uncovered. 1 pc
visible light infrared protostars not seen in visible light Remember: longer wavelength radiation is not so easily absorbed by dust!
Newly formed stars in Orion with Protoplanetary Disks (Hubble)
Star Clusters Two kinds: 1) Open Clusters -Example: The Pleiades -10's to 100's of stars -Few pc across -Loose grouping of stars -Tend to be young (10's to 100's of millions of years, not billions, but there are exceptions)
2) Globular Clusters - few x 10 5 or 10 6 stars - size about 50 pc - very tightly packed, roughly spherical shape - billions of years old Clusters are crucial for stellar evolution studies because: 1) All stars in a cluster formed at about same time (so all have same age) 2) All stars are at about the same distance 3) All stars have same chemical composition
Clicker Question: A giant protostar of 100 Rsun is heated by what process? A: burning of chemical elements B: nuclear fission C: gravitational collapse D: nuclear fusion
Clicker Question: Star formation in the ISM today happens most often: A: In the Oort cloud. B: In dense molecular clouds. C: In the central parsecs of the Galaxy. D: In globular clusters
Stellar Evolution: Evolution off the Main Sequence Main Sequence Lifetimes Most massive (O and B stars): millions of years Stars like the Sun (G stars): billions of years Low mass stars (K and M stars): a trillion years! While on Main Sequence, stellar core has H -> He fusion, by p-p chain in stars like Sun or less massive. In more massive stars, “CNO cycle” becomes more important.
Evolution of a Low-Mass Star (< 8 Msun , focus on 1 Msun case) - All H converted to He in core. - Core too cool for He burning. Contracts. Heats up. - H burns in shell around core: "H-shell burning phase". - Tremendous energy produced. Star must expand. - Star now a "Red Giant". Diameter ~ 1 AU! - Phase lasts ~ 109 years for 1 MSun star. - Example: Arcturus Red Giant
Eventually: Core Helium Fusion - Core shrinks and heats up to 108 K, helium can now burn into carbon. "Triple-alpha process" 4He + 4He -> 8Be + energy 8Be + 4He -> 12C + energy - First occurs in a runaway process: "the helium flash". Energy from fusion goes into re-expanding and cooling the core. Takes only a few seconds! This slows fusion, so star gets dimmer again. - Then stable He -> C burning. Still have H -> He shell burning surrounding it. - Now star on "Horizontal Branch" of H-R diagram. Lasts ~108 years for 1 MSun star.
More massive less massive Horizontal branch star structure Core fusion He -> C Shell fusion H -> He
Helium Runs out in Core • All He -> C. Not hot enough • for C fusion. - Core shrinks and heats up. - Get new helium burning shell (inside H burning shell). - High rate of burning, star expands, luminosity way up. - Called ''Red Supergiant'' (or Asymptotic Giant Branch) phase. - Only ~106 years for 1 MSun star. Red Supergiant
"Planetary Nebulae" - Core continues to contract. Never gets hot enough for carbon fusion. - Helium shell burning becomes unstable -> "helium shell flashes". - Whole star pulsates more and more violently. - Eventually, shells thrown off star altogether! 0.1 - 0.2 MSun ejected. - Shells appear as a nebula around star, called "Planetary Nebula" (awful, historical name, nothing to do with planets).
NGC2438 AAT 3.9m 1.5 GHz VLA image from Taylor & Morris
Bipolar Planetary nebulae
White Dwarfs - Dead core of low-mass star after Planetary Nebula thrown off. - Mass: few tenths of a MSun . -Radius: about REarth . - Density: 106 g/cm3! (a cubic cm of it would weigh a ton on Earth). - White dwarfs slowly cool to oblivion. No fusion.