Chapter 17: Evolution of High-Mass Stars

1. Chapter 17: Evolution of High-Mass Stars

2. Massive stars have more hydrogen to start with but they burn it at a prodigious rate The overall reaction is still There are 3 gamma ray photons instead of two and it consumes hydrogen muchfaster but requires higher temperatures.

3. High-mass stars have convection in their cores Because of convection in their core, high mass stars never develop a degenerate helium core so they never have a helium flash.

4. As high mass stars evolve off the main sequence they move back and forth on the H-R diagram

5. For high-mass stars the core temperature will get hot enough to fuse carbon Carbon will start fusing when the core temperature reaches 800,000,000 Kelvin. Unlike hydrogen fusion which only produces helium or helium fusion which only produces carbon, carbon fusion can produce lots of different elements.

6. As the temperature gets higher, heavier elements start to fuse The products of one fusion will form the elements for the next level of fusion making the core start to look like an onion with multiple shells of fusion

7. As they evolve, some stars move into the “instability strip” In the instability strip stars can begin to pulsate. The first pulsating star to be discovered was Delta Cephei so we call this type of star a Cepheid variable

8. For Cepheid variables, the brightness varies in a regular way

9. Another type of pulsating variable is RR Lyrae

10. The pulsations are due to a layer of helium that becomes ionized

11. The period of their variation is related to their luminosity

12. Once an iron core starts to form, the end comes quickly

13. Each stage of fusion requires higher temperatures, releases less energy and lasts less time

14. Higher fusion also releases most of its energy as neutrinos Since neutrinos don’t interact with normal matter much, they quickly escape the star and don’t help in balancing the inward crush of gravity.

15. Because of the nuclear force, fusing iron requires energy rather than releasing it

16. At this point temperature in the core is nearly 5 billion K The peak of the blackbody curve that is being produced is in the high energy gamma ray range

17. Due to degeneracy, extreme temperature and pressure, the core starts to collapse Once the iron becomes degenerate, the core starts to collapse as more mass is added. As it collapses, it gets hotter. As it gets hotter, the gamma rays get more energetic until they have enough energy break up the iron. The process is called photodisintegration g+ 56Fe→134He + 4n

18. After photodisintegration, reverse beta decay relieves the electron degeneracy pressure Things get so crowded the electrons are squeezed into the nucleus where they combine with protons to make neutrons in a process called Reverse Beta Decay

19. Reverse Beta Decay causes neutrinos to pour out of the core The conversion of electrons and protons into neutrons causes the core to rapidly shrink in size which produces a blast of heat which forms a shock wave. In addition, huge amounts of energy is being carried off by the neutrinos

20. The shock wave pushes the rest of the star outward

21. The result is a Type II Supernova

22. Supernovae come is several types Type Ib through Type II are from the core collapse of a massive star. Type Ia is the thermonuclear detonation of a white dwarf star.

23. The last naked-eye supernova was SN 1984A The first supernova to be observed in 1987, it was visible to the naked eye for several weeks if you were in the southern hemisphere. It occurred in the Large Magellanic Cloud, a satellite galaxy 180,000 ly away.

24. Type II Supernovae are important for the elements they produce

25. The Solar System formed from the debris of several supernovae

26. After the supernova, a neutron star is left behind Because of the peculiarities of their emissions, they are called Pulsars

27. Pulsars are spinning Neutron Stars The Lighthouse Model

28. The Crab pulses in all wavelengths

29. Pulsars emit by synchrotron radiation Charged particles spiraling in a magnetic field produce synchrotron radiation. The stronger the magnetic field, the shorter the wavelength emitted

30. If a pulsar is radiating, where is the energy coming from?

31. Pulsars in a binary system will emit x-rays and gamma rays

32. How do we know all this stuff about stellar evolution? Since the stars in a cluster are all born at about the same time, we can study clusters to learn how stars evolve

33. The H-R Diagram of a cluster shows which stars are starting to evolve off the main sequence

34. The actual H-R diagram of clusters match the theory very well

35. By comparing clusters of different ages we can understand how stars evolve