lecture 17 post-ms evolution ii. review review review

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Lecture 17 Lecture 17 Post-ms evolution II

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Page 1: Lecture 17 Post-ms evolution II. Review Review Review

Lecture 17Lecture 17

Post-ms evolution II

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ReviewReview

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Second dredge-up: He-shell burningSecond dredge-up: He-shell burning

•A Helium-burning shell ignites around a C,O core. Similar to the H-shell burning phase

•Again, the envelope expands and cools, becoming convective and causing a second dredge-up.

Instability strip

Page 6: Lecture 17 Post-ms evolution II. Review Review Review

Review: Horizontal branchReview: Horizontal branch

•H-burning shell is compressed, increasing the luminosity it produces

•He-shell burning: CO core collapses, while envelope expands

Start of HBEnd of HB

He →C,O burning

Convection

H →He burning

Page 7: Lecture 17 Post-ms evolution II. Review Review Review

Asymptotic giant branchAsymptotic giant branch

As the envelope cools it eventually reaches the Hayashi track and bends upward. This is the asymptotic giant branch.

He-burning dominates the luminosity

Page 8: Lecture 17 Post-ms evolution II. Review Review Review

Thermal pulsesThermal pulses

•He ash is dumped on the slightly degenerate He-burning shell, causing shell flashes

Page 9: Lecture 17 Post-ms evolution II. Review Review Review

Further nucleosynthesisFurther nucleosynthesis

For stars with 4<M/MSun<8, nuclear reactions can continue:

pNa

nMg

HeNe

HeO

CC

2311

2312

42

2010

42

168

126

126

2

nS

pP

HeSi

HeMg

OO

3116

3115

42

2814

42

2412

168

168

2

Page 10: Lecture 17 Post-ms evolution II. Review Review Review

AGB starsAGB stars

•High mass-loss rates, and cool effective temperatures (~3000 K)

•A dust shell hides most of the stellar luminosity and so the stars are seen only in the infrared.

Page 11: Lecture 17 Post-ms evolution II. Review Review Review

Mass lossMass loss

•Mass loss driven by the high luminosity and thermal pulses.

As mass decreases, and luminosity increases, the mass loss rate increases.

High-resolution radio image of mass-loss from an AGB star, TX Cam

Page 12: Lecture 17 Post-ms evolution II. Review Review Review

BreakBreak

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Post-AGB phasePost-AGB phase

• The cloud expands and becomes optically thin• Exposes the hotter interior

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Planetary nebulae: Fate of low mass Planetary nebulae: Fate of low mass starsstars

• The hot core lights up the expanding envelope, for about 20,000 years.

Page 15: Lecture 17 Post-ms evolution II. Review Review Review

Planetary NebulaePlanetary Nebulae

•Bluish-green colour due to [OIII] forbidden lines•Reddish colour from ionized hydrogen and nitrogen

Cat’s eye nebula

Page 16: Lecture 17 Post-ms evolution II. Review Review Review

The Helix NebulaThe Helix Nebula

•Looking along the rotation axis Gas is being ejected in “rings” preferentially along the

equator

Page 17: Lecture 17 Post-ms evolution II. Review Review Review

Outflow velocitiesOutflow velocities

•Typically shell expands at 10-30 km/s•Some are much faster: the Ant nebula has an outflow velocity of about 1000 km/s

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Fate of planetary nebulaeFate of planetary nebulae

•Release the envelope into the ISM, on a timescale of ~10000 years.

•There are probably about 15,000 in the Milky Way today ISM is being enriched at a rate of about 1 Msun/year.

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Planetary nebulae and white dwarfsPlanetary nebulae and white dwarfs

• When the helium and hydrogen shells are extinguished, the luminosity drops abruptly

Page 20: Lecture 17 Post-ms evolution II. Review Review Review

White dwarfsWhite dwarfs

•When the envelope has dispersed, only the hot, dense, small core is left