stellar evolution for low mass stars
DESCRIPTION
Evolution of low mass stars on the main sequenceTRANSCRIPT
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Stellar EvolutionSolar Mass Stars
Overview
How and Why stars evolve off the MS?
Life on the Main Sequence
Evolutions depends on Mass
Will focus on Sun Type Stars today
Sun is a fairly average star A Low Mass Star
Overview
Stages of evolution of a Low Mass Star
Main Sequence Star
Red Giants Processes in the Core & on the Surface
Helium Flash to Horizontal Branch (HB)
HB to Asymptotic Giant Branch
Planetary Nebula & White Dwarfs
Main Sequence Stars are Stable
Energy Balance :
Energy lost at the surface (Luminosity)
Energy of fusing H into He at the stars core.
Pressure (push) counters Gravity (pull):
Reaction rates are Temperature dependent
Too high - core heats up and then expands
Expansion cools the core, so reaction rates get slower.
Too small - core cools off and then shrinks
Shrinking heats the core, so reaction rates get faster.
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Main Idea Life on the Main Sequence
A nice Pressure-Temperaturefeedback mechanism, keeps the
stars Luminosity constant.
Main Sequence Stars are Stable
What happens to the He created by H fusion
Core is too cool to ignite He fusion
Slowly builds up an inert He core
Main Sequence (H-burning) Lifetime
10 Gyr for 1Msun star (eg. Sun)
10 Tyr for 0.1Msun star (red dwarf)
Stellar Evolution
Main sequence stars are just a part of a bigger
picture
Stellar evolution depends of the stars mass
Massive stars burn more quickly,
Therefore, evolve more quickly
Four final states: White Dwarfs, Neutron Stars,
Black Holes and Nothing!
Main-Sequence Evolution 41
1 24 during the MS lifetime
Number density of the particles drop with time
Pressure drops Core contracts (Why?)
Core Contracts core Temperature rises Fusion rates go up
Stars Luminosity will go up with time
Star will expand somewhat (Why?)
Surface opacity keeps Temperature same
L 24
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Stars evolve, even on the Main-Sequence
Lum
inosity (
Lsu
n)
O B A F G K M
Zero Age
Main-Sequence
TemperatureRef: Seeds
30 M
3 M
Initial Sun
Present Sun
1010 yrs
6x108 yrs
5x106 yrs
Stage 1: Life on the Main Sequence
5 billion years ago:
Beginning of its life on main-sequence
Sun had 70% luminosity it has now.
5 billion years from now:
End of its life on main-sequence
Sun will have twice the luminosity it has now.
At some point, the oceans will boil
Whats happening Inside
He created by H-fusion in the core
Slowly builds up He core
But, core is too cool to ignite He fusion
Eventually, Hydrogen in the core is exhausted
Gravity starts winning He core collapses & heats up
H-burning in a Thin Shell surrounding the core
MS (H He in core): 90% of lifetime
Whats happening Outside
H-fusion in the shell surrounding core
Collapsing core heats up this shell
Hotter shell faster fusion
H-burning shell drives expansion of the Envelope
Pressure starts winning Envelope expands & cools
Star gets Brighter & Redder
Creates a Red Giant/Supergiant
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Inert He
Core
H-Burning Shell
Cool, Extended Envelope
Some Real Stars
Stage 2: Red Giants
Sun like stars expand to 10-100 r
e.g. Arcturus (26 r)
O Stars expand upto 1000 r
~ 5 AU = Jupiters Orbit!
e.g. Mira (Omicron Ceti)
Takes about 1Gyr to climb up RGB
He core contracting & Heating but no fusion
Whats happening Outside
At the surface very low density of material.
Surface cools to 3000-3500K by ion opacity feedback mechanism
Opacity slows the heat flow, regulates temperature
Too cool metals are not ionized: +
breaks down Opacity goes down Temperature rises
Too hot metals ionize: +
Too much Opacity goes up Temperature goes down
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Whats happening Inside
Heat source is not the core
Gravity winning in the core Contraction
Shell gets hotter Increases H-burning in shell Luminosity
But, surface temperature maintained constant
L 24
This stage marked by variability and L~ 103
Mass loss from surface possible as gravity is weak
Whats happening Inside
Near the end of the red-giant stage, the core is very small
compared with the envelope
Like comparing a Baseball to the Stadium
But, the core contains most of the Mass
~ 12% but
Density is large ~ 1000 g/cm3
1 Coffee cup ~1300 lbs, thats one strong cup!
At the tip of the RGB: reaches 100 Million K Helium
Flash
Degenerate Matter
At high densities, quantum effects become important
Electrons are only allowed in discrete states, and no two electrons can
occupy the same state
High density lots of e-/cm3 degenerate matter
Electrons are trapped in certain states
Forming an energy level stack: low to high
Degenerate Matter resists Compression
Pressure becomes independent of Temperature
This Degeneracy Pressure can now support the Core
Degenerate Matter
What if we add energy to degenerate matter?
Cant change Pressure! Cant compress/expand!
All the Energy absorbed by particles large velocities,
Here, the electrons become degenerate
Electron Degeneracy Pressure, important in:
Helium cores of Red Giant Stars
Stellar end states of White Dwarfs
Will later see neutron degeneracy pressure in Neutron Stars
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Cool, Extended EnvelopePossible Mass Loss
Main Sequence Star
Red Giant Star
He core supported by degeneracy Pressure
Stage 3: The Helium Flash Core supported by reaches 10
8
New Fusion Source takes over the Triple- Process ( 4 12)
Starts He fusion! Fusion Rate 40
For Massive stars (> 3)
Core contracts quickly, Degeneracy plays small role
He fusion starts smoothly, No Helium flash
For Less Massive stars (0.4 3)
Core contracts slowly, Degeneracy is important
Density goes to 105g/cm3. He fusion starts at the Flash!
Stars < 0.4 DO NOT burn Helium at all
Whats happening
Star generates 1011 for a few seconds - More than the Galaxy!
Huge Energy from He-flash, relieves degeneracy pressure
Expands the Core, restores Pressure-Gravity Balance
Inside:
He burning in the core via Triple- Process
Additional H burning in the shell surrounding the core
Outside:
Star gets Hotter & Bluer, also Shrinks in Radius
Luminosity Drops, Leaves RGB Moves to Horizontal Branch
He Burning
Core
H-Burning Shell
Envelope
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Stage 4: The Horizontal Branch
Can be thought as the He-burning Main Sequence
Energy generated in core = Energy lost at surface through Luminosity
P-T feedback mechanism star is stable
On the HB, Energy is derived from:
He-burning in the Core and H-burning in the shell
L ~ 30 100
Whats happening Inside
Carbon created by He-fusion in the core
Triple- Process is comparatively inefficient, Slowly builds up C-core
But, core is too cool to ignite Carbon fusion
Eventually, Helium in the core is exhausted
Gravity starts winning, C core collapses & heats up
He-burning in a Thin Shell surrounding the C core
H-burning in a Shell outside the He burning shell
Horizontal Branch (He-burning) Lifetime
~ few 100 Million Years
Whats happening Outside
H & He-fusion in shells surrounding Carbon core
Collapsing core heats up these shells
Hotter shell sustain fusion
Pressure starts winning Envelope expands & cools
Star gets Brighter & Redder
But, remember He fusion requires higher temperature
This time the star has a higher effective Temperature
Climbs up the Asymptotic Giant Branch
Inert Carbon
Core
He-Burning Shell
Cool, Extended Envelope
H-Burning Shell
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Stage 5: The Asymptotic Giant Branch
Core Envelope Separation
H & He-shell burning drives Luminosity
Eventually, Radiation Pressure drives away the outer envelope
Rapid Process, takes ~ 105yrs
Expanding envelope forms a nebula around the contracting Core
Planetary Nebula
Whats happening
For a star like Sun, the core continues to contract
But, now mass of the envelope is gone
Less gravity to push, ,
Until supported by electron degeneracy pressure
White Dwarfs
It never gets hot enough to fuse Carbon (600 Million K)
More massive stars will use these elements
More catastrophic endings
White Dwarf
Planetary Nebula
Stage 6: Planetary Nebula & White Dwarfs The hot core remains and becomes a White Dwarf
Mass ~ 1 & Radius ~
Supported by degeneracy pressure
Stars with 0.4 3end up producing Planetary Nebula & White
Dwarfs
This is our Suns future
Stars upto 8 can gracefully exit this way due to Mass Loss
Even less massive stars (Red Dwarfs) can live on the Main sequence
for longer than the age of the Universe
Eventually become Black Dwarfs, as H-shell burning never starts
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Stage 6: Planetary Nebula & White Dwarfs
Planetary Nebula: Look like Planets
But they are not - Ofcourse, you knew that!
Many examples Pretty Pictures following
~ 10 30 km/s & Radius ~ 0.3 pc
Ages ~ 10,000 , vanish in ~ 50,000
Mass ~ 0.5
About 1500 known, ~ 50,000 estimated in Galaxy
Planetary Nebula: WD at Center of NGC 2440 (HST)
Planetary Nebula: Ring Nebula (HST) Planetary Nebula: NGC 3132 (HST)
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Planetary Nebula: Helix Nebula Planetary Nebula: IC 418 (HST)
Planetary Nebula A39: Optical Planetary Nebula: IC 3568 Lemon Slice Nebula (HST)
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Planetary Nebula: Owl Nebula (HST) Planetary Nebula: M27
Planetary Nebula: Dumbbell (VLT) Planetary Nebula: NGC 6751 (HST)
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Planetary Nebula: NGC 6751 Zoomed in (HST) Planetary Nebula: Red Rectangle
Planetary Nebula: NGC 7027 (HST) Planetary Nebula: Stingray (HST)
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Planetary Nebula: M2 Butterfly Nebula in the Visible : VLT
Planetary Nebula: CRL 2688 Egg Nebula Planetary Nebula: Egg Nebula in NIR
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Planetary Nebula Planetary Nebula: NGC 7009 Saturn Nebula (HST)
Planetary Nebula: Cats Eye Nebula (HST) Planetary Nebula: Etched Hourglass (HST)
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Sirius A and B
Optical X-rays