Lecture 10: A Star is Born- 7 Easy Steps to Thermonuclear Ignition

"The heavens call to you, and circle around you, displaying to you their eternal slendours, and your eye only gazes to earth."

Dante, Purgatorio



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  • Date: February 28, 1995
    Reading Assignment: pp. 433-443

    Description : theoretical overview of star formation

    Objectives

  • be able to describe how heat, rotation, and magnetism hinder star formation
  • be able to explain why gravity eventually overcomes heat causing stars to form
  • be able to describe the concept of an evolutionary track
  • be able to describe conditions at the beginning of star formation
  • be able to describe the fragmentation inside an interstellar cloud and why it occurs
  • be able to describe the formation of a protostar
  • be able to explain Kelvin-Helmholtz contraction of a protostar and the changes that take place in the luminosity and temperature of the star
  • be able to describe the Hayashi track and the changes that take place in the luminosity and temperature of the star
  • be able to describe why nuclear burning begins in the star
  • be able to describe the final adjustments the star makes when it moves onto the main sequence
  • be able to describe how the stars final mass affects the speed in which it forms

  • Lecture Outline

    Slide # 1: A Star is Born

  • 7 Easy Steps to Thermonuclear Ignition
  • Slide # 2: The HR Diagram (GRAPHICS)
  • Why?
  • Slide # 3: Unanswered Questions
  • Why are 90% of stars on the Main Sequence?
  • Why is mass so important in determining luminosity?
  • How can a 1 solar mass star be a red giant, white dwarf, or on the main sequen
  • Why are red giants and white dwarfs different than MS stars?
  • Slide # 4: Star Modeling- Laws of Physics
  • hydrostatic equilibrium
  • energy transport
  • energy generation
  • mass continuity
  • Slide # 5: Evolutionary Tracks
  • every star corresponds to place on the HR diagram at any given time
  • stars may change luminosity or temperature over their lifetime
  • stars may follow tracks on the HR diagram
  • Slide # 6: The HR Diagram (GRAPHICS)
  • one solar mass star over 8 billion years
  • Slide # 7: Gravity Causes Collapse
  • gravity in a gas cloud may cause it to contract
  • Slide # 8: Forces the Oppose Contraction
  • gas pressure and heating
  • hydrostatic equilibrium
  • rotation
  • rotation flattens the system
  • opposes collapse
  • magnetic fields
  • rapidly strengthens with contraction
  • Slide # 9: Hydrostatic Equilibrium (GRAPHICS)
  • a balance between pressure and gravity
  • Slide # 10: Hydrostatic Equilibrium
  • most stars are in hydrostatic equilibrium
  • they are not expanding or contracting
  • gravity and pressure are balanced
  • forming stars ARE NOT in hydrostatic equilibrium
  • they are contracting
  • gravity is overcoming pressure
  • Slide # 11: Rotation (GRAPHICS)
  • angular momentum opposes collapse
  • rotation speeds up as the system collapses
  • Slide # 12: Magnetic Fields (GRAPHICS)
  • compression increases magnetic fields
  • stronger magnetic fields oppose compression
  • Slide # 13: A Simplification
  • the most important effect is pressure
  • gas pressure and heat
  • ignore rotation and magnetic fields
  • probably less important
  • Slide # 14: Pressure and Gravity
  • gas pressure is caused by moleculer motion
  • heating causes molecular motion
  • collapse causes heating
  • Slide # 15: How does collapse take place?
  • more compression means more heat
  • more heat means more pressure
  • so how does it collapse?
  • Slide # 16: Cooling of the Gas
  • higher density means more interactions between particles
  • more interactions mean more radiation
  • more radiation means more cooling
  • Slide # 17: Cooling (GRAPHICS)
  • cooling must occur before a star is formed
  • Slide # 18: Two Competing Effects
  • cooling - energy is radiated
  • heating - pressure increases
  • Slide # 19: Star Formation
  • 7 basic steps to forming stars
  • examine formation of a ONE SOLAR MASS star
  • Slide # 20: The Steps
  • gas cloud
  • fragmentation
  • protostar
  • Helmholtz contraction
  • Hayashi track
  • ignition
  • adjustment to the Main Sequence
  • Slide # 21: Stage 1: Gas Clouds
  • high density HI or H2 region
  • 1000 particles per cubic cm
  • 10 parsecs in size
  • 10 K temperature
  • often Molecular Clouds
  • a bit cooler and denser than most of the ISM
  • 1 particle per cubic cm
  • 100 K temperature
  • Slide # 22: Molecular Clouds
  • temperature = 20K
  • ISM is normally 100K
  • density = 106 atoms per cubic cm
  • ISM has a density of 1 atom per cubic cm
  • most gas is molecular hydrogen (H2)
  • ISM is mostly HI gas
  • Slide # 23: Molecular Cloud Composition
  • almost all gas is molecular Hydrogen (H2)
  • very little HI
  • interstellar dust grains
  • 1 part in 1012
  • one part in a million or billion is other molecules
  • 60 detected in interstellar space
  • Slide # 24: The ISM (GRAPHICS)
  • molecular clouds
  • Slide # 25: Stage 2: Fragmentation
  • cloud breaks into pieces
  • 2 solar masses of material
  • 10 6 particles per cubic cm
  • few one-hundreth's of a parsec
  • few hundred times the size of solar system
  • 100 K temperature
  • Slide # 26: Fragmentation (GRAPHICS)
  • big cloud breaks into many little clouds
  • Slide # 27: Stage 3: Protostar
  • gas cloud heats up
  • radiation becomes trapped
  • size of the solar system
  • 10,000 times the size of the Sun
  • temperature reaches 10,000 K at the core
  • density 1012 particles per cubic cm
  • age = 10,000 years
  • photosphere forms
  • gas becomes opaque
  • Slide # 28: Protostar (GRAPHICS)
  • photosphere forms
  • Slide # 29: Constellation Corner (GRAPHICS)
  • Constellation De Jour
  • Slide # 30: Gemini (GRAPHICS)
  • Feb 15 - 9pm - S - 4.0
  • Slide # 31: Gemini (GRAPHICS)
  • Feb 15 - 9pm - S - 4.0
  • Slide # 32: Gemini (GRAPHICS)
  • Feb 15 - 9pm - S - 5.0
  • Slide # 33: Stage 4: Kelvin-Helmholtz Contraction
  • protostar contracts and heats up
  • core temperature = 1,000,000 K
  • surface temperature = 3,000 K
  • size = 50 solar radii
  • no nuclear reactions yet
  • very luminous - more than 1,000 solar luminosity
  • age = 100,000 years
  • star can be plotted on HR diagram
  • appears in red giant area
  • Slide # 34: The HR Diagram (GRAPHICS)
  • HR diagram
  • Slide # 35: Stage 5: Hayashi Track
  • star contracts, surface temperature rise a small amount
  • 10 times the size of the Sun
  • surface temperature 4000 K
  • luminosity = 10 solar luminosity
  • central temperature = 5,000,000 K
  • no nuclear reactions
  • age = 1 million years
  • luminosity decreases as star shrinks
  • Slide # 36: The HR Diagram (GRAPHICS)
  • HR diagram
  • Slide # 37: Stage 6: Nuclear Ignition
  • P-P Chain Begins in the Core
  • core temperature > 10,000,000 K
  • surface temperature 4,500 K
  • size = 1.25 solar radii
  • luminosity = 2/3 solar luminosity
  • age = 10 million years
  • star still not in hydrostatic equilibrium
  • internal structure slightly out of balance
  • Slide # 38: The HR Diagram (GRAPHICS)
  • HR diagram
  • Slide # 39: Stage 7: Adjustments to Main Sequence
  • star moves to main sequence
  • star is now a G2V
  • 15,000,000 K core temperature
  • one solar luminosity
  • 6,000 K surface temperature
  • central density = 100 gm/cm3
  • age = 40 million years
  • star in hydrostatic equilibrium
  • Slide # 40: The HR Diagram (GRAPHICS)
  • HR diagram
  • Slide # 41: Emission Nebula (GRAPHICS)
  • M42 - the Orion Nebula - an HII region
  • Slide # 42: Nebula (GRAPHICS)
  • M20 - the Trifid Nebula
  • emission, absorption, and reflection
  • Slide # 43: Effects Interstellar Dust
  • stars appear redder
  • absorbs blue light more than red
  • appear dimmer
  • absorbs visible light
  • star light is polarized
  • Slide # 44: How do we observe star formation?
  • found in molecular clouds
  • lots of dust
  • Slide # 45: Emission and Excitation
  • transition between orbitals
  • produces most visible line emission
  • spin-flip of electron
  • HI gas- 21cm line emission (radio)
  • rotational excitation
  • molecular emission - radio
  • thermal emission
  • peak of stars is in the visible range
  • peak of protostars is in the infrared