Top Banner
Stellar Evolution II
19

Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Mar 26, 2015

Download

Documents

Amelia Sweeney
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Stellar Evolution II

Page 2: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

The Upper End of the Main Sequence:How massive can a star get?

• Larger clouds of gas (GMCs) tend to fragment into smaller ones before collapsing to form stars – very massive stars are rare• Stars with masses above 50 MSUN are unstable – nuclear reactionsin their core produce energy at such a fast rate that they blow offtheir outer layers, losing mass.

Page 3: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Eta Carinae

• Mass: 100-150MSUN

• Giant eruption in 1843Made it 2nd brightest starin sky for a short time•Created two giant lobesof hot gas expanding awayfrom the star

Page 4: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Evolution of Stars on the Main Sequence• Core starts with same fraction of

hydrogen as whole star• Fusion changes H He• For each reaction, the star loses 4

H and gains only one He, so pressure decreases and gravity squeezes the core more tightly

• Core gradually shrinks and gets hotter, increasing the pressure to compensate

• Energy generation rate gradually increases, so star gets more luminous and the surface gets hotter. Increased pressure of radiation increases the radius.

H > He

Page 5: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Evolution of Stars on the Main Sequence

Page 6: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Evolution of Stars on the Main Sequence• Lifetime of stars on the main sequence:

• More massive stars burn their fuel faster, so will use it upquicker > have smaller lifetimes• Lifetime T = 1/M2.5

• O5 - 1,000,000 yr• A0 - 440,000,000 yr• G0 - 8,000,000,000 yr• K0 - 17,000,000,000 yr• M0 - 56,000,000,000 yr

• (age of universe: 13,600,000,000 yr)

Page 7: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Main Sequence Stars:• Energy generated by fusing H to He in their core• Luminosity and surface temperature increase as mass increases

Page 8: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Post-MS Evolution of Low Mass Stars(M < 8MSUN)

H > He

• What happens when the core runs out of Hydrogen?

H

Page 9: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Post-MS Evolution of Low Mass Stars(M < 8MSUN)

• Core stops producing energy – gravity causes it to contract and heat up

He

• Layer surrounding the core also contracts and heats up enough to start fusing H to He

H > He• Outer parts of star expandbecause star is H – burning layeris producing more energy than is required to balance gravity

• Surface gets cooler because ofincreased area > star becomes redgiant

Page 10: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Post-MS Evolution of Low Mass Stars(M < 8MSUN)

Page 11: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Post-MS Evolution of Low Mass Stars(M < 8MSUN)

Page 12: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Degenerate Gases

Normal Gas:• Compress normal gases > particles move faster > increased pressure and temperature

• Heat a normal gas > pressure increases

Page 13: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Degenerate Gases:• If gas is dense enough, particles have no where to move – if you compress the gas, the particles cannot move faster; they simply ‘wiggle’ more energetically• Compress degenerate gas > temperature increases but pressure remains the same• Heat a degenerate gas > pressure stays the same

Degenerate Gases

Page 14: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Flash• Matter in core is fully ionized – all electrons are free of their atoms• Most pressure in the core is from the electrons• As the core of Helium ash shrinks, it becomes degenerate – its temperature will increase but its pressure will remain the same• Density now around 1000,000 grams/cubic cm (about 1000 tonnes/cc)• As the temperature of the core passes 100,000,000 K, it can start Hefusion into Carbon

Page 15: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Flash• He ignites > produces energy > temperature increases, but pressurestays the same – the core cannot respond to the increased temperatureby expanding• Increases temperature > increased He fusion rate > increased energyproduction > increased temperature > increased He fusion rate > increased energy production > increased temperature > increased He fusion rate > increased energy production > increased temperature > ....

• Explosion! – the HeliumFlash

Page 16: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Flash• For a few minutes the core generates 100,000,000,000,000 timesmore energy per second than the sun – 100 times more energy persecond than all the stars in the Milky Way combined• Does not destroy the star – energy is absorbed in outer layers. Nooutward sign of explosion• Helium flash only occurs in stars between 0.5 and 3 MSUN • After a few minutes, the core becomes so hot that the gas becomesnormal again, and pressure increases

Page 17: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Burning

He > C, O

H > He

• He fused to C, O in core• H still fusing to He in shell around core

Page 18: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Burning

He > C, O

H > He

• Extra energy from He Fusion causes core to Expand• This forces H burning shell to expand.

Page 19: Stellar Evolution II. The Upper End of the Main Sequence: How massive can a star get? Larger clouds of gas (GMCs) tend to fragment into smaller ones before.

Helium Burning

He > C, O

H > He

• Expansion cools H burning shell, which then absorbs heat from the envelope, causing it to shrink a little and get hotter