1. PHYS 3380 - Astronomy Protostellar Disks and Jets – Herbig Haro Objects Disks of matter accreted onto a protostar (“accretion disks”) often lead to the formation of jets (directed outflows; bipolar outflows) - originate from the star and the inner parts of the disk and become confined to a narrow beam within a few billion miles of their source. - not known how the jets are focused, or collimated. Suggested that magnetic fields, generated by the star or disk, might constrain the jets. When they strike interstellar medium/nebula - produce Herbig Haro Objects - small nebulae that fluctuate in brightness

2. PHYS 3380 - Astronomy Protostellar Disks and Jets – Herbig Haro Objects HH34 Almost 50 years ago, George Herbig and Guillermo Haro independently discovered a number of compact nebulae with peculiar spectra near dark clouds. - subsequently demonstrated that these objects were shock- excited nebulae. - shown that the large range of excitation conditions requires bow shocks and other complex morphologies. By the early 1980s, several Herbig-Haro (HH) objects shown to be highly collimated jets of partially ionized plasma moving away from young stars at speeds of 100 to over 1000 km/s.

3. PHYS 3380 - Astronomy Stellar Jets Of the 56 proplyds observed in the Orion nebula, 23 had visible jets.

4. PHYS 3380 - Astronomy Gases clumped - could provide insights into the nature of the disk collapsing onto the star. Beaded jet structure "ticker tape" recording of how clumps of material have, episodically, fallen onto the star. jets "wiggle" along their multi-trillion-mile long paths, suggesting the gaseous fountains change their position and direction. - might be evidence for a stellar companion or planetary system that pulls on the central star, causing it to wobble, which in turn causes the jet to change directions knots due to 'sputtering' of the central engine Ubiquitous in the universe - occur over a vast range of energies and physical scales, in a variety of phenomena. Stellar Jets HH30

5. PHYS 3380 - Astronomy Protostellar Disks and Jets – Herbig Haro Objects Herbig Haro Object HH30

6. PHYS 3380 - Astronomy XZ Tauri - young system with two stars orbiting each other - separated by about 6 billion kilometers (about the distance from the Sun to Pluto) - shows bubble of hot, glowing gas extending nearly 96 billion kilometers from this young star system. - appears much broader than the narrow jets seen in other young stars, but it is caused by the same process - the ejection of gas from a star. XZ Tauri

7. PHYS 3380 - Astronomy Evidence of Star Formation Nebula around S Monocerotis: Contains many massive, very young stars - O associations Also includes T Tauri Stars – generally low mass stars, strongly variable; bright in the infrared - T associations Fox Fur Nebula Observe regions containing young stars - must have formed recently - lie between birth line and main sequence Regions of star formation rich in dust and gas and contain IR protostars and stars still contracting toward the main sequence

8. PHYS 3380 - Astronomy Low-mass star formation in upper Scorpius - dashed lines evolutionary tracks of observed low-mass stars - all the low-mass PMS (pre-main sequence) stars have a mean age of about 5 Myr and show no evidence for a large age dispersion. - thin solid lines isochrones at 0.1, 0.3, 1, 3, 10, 30 Myr Main Sequence

9. PHYS 3380 - Astronomy Evidence of Star Formation The Cone Nebula Optical Infrared Young, very massive star Smaller, sunlike stars, probably formed under the influence of the massive star Stellar formation itself triggers star evolutions - massive stars’ ionization fronts compress nearby gasses - trigger

10. PHYS 3380 - Astronomy Evidence of Star Formation Star Forming Region RCW 38

11. PHYS 3380 - Astronomy Open Clusters of Stars Large masses of Giant Molecular Clouds => Stars do not form isolated, but in large groups, called Open Clusters of Stars. Open Cluster M7

12. PHYS 3380 - Astronomy Open Clusters of Stars Large, dense cluster of (yellow and red) stars in the foreground; ~ 50 million years old Scattered individual (bright, white) stars in the background; only ~ 4 million years old

13. PHYS 3380 - Astronomy Globules ~ 10 to 1000 solar masses; Contracting to form protostars Bok Globules:

14. PHYS 3380 - Astronomy Globules Evaporating Gaseous Globules (“EGGs”): Newly forming stars exposed by the ionizing radiation from nearby massive stars - Shadows of the EGGs protect gas behind them, resulting in the finger-like structures at the top of the cloud. - Forming inside at least some of the EGGs are embryonic stars -- abruptly stop growing when the EGGs are uncovered - separated from the larger reservoir of gas from which they were drawing mass. Eventually emerge as the EGGs themselves succumb to photoevaporation. The pillar is slowly eroding away by the ultraviolet light from nearby hot stars - "photoevaporation". As it does, small globules of especially dense gas buried within the cloud are uncovered.

15. PHYS 3380 - Astronomy

16. Stellar Evolution

17. PHYS 3380 - Astronomy Stellar Types by Mass Brown dwarfs (and planets): estimated lower stellar mass limit is 0.08 M  (or 80M Jup ). Lower mass objects have core T too low to ignite H. Red dwarfs: stars whose main-sequence lifetime exceeds the present age of the Universe (13.7x10 9 yr). Models yield an upper mass limit of stars that must still be on main-sequence, even if they are as old as the Universe of 0.7M  Low-mass stars: stars in the region 0.7 ≤ M ≤ 2 M . After shedding considerable amount of mass, they will end their lives as white dwarfs and possibly planetary nebulae. Intermediate mass stars: stars of mass 2 ≤ M ≤ 8-10 M . Similar evolutionary paths to low-mass stars, but always at higher luminosity. Give planetary nebula and higher mass white dwarfs. High mass (or massive) stars: M >8-10 M . Distinctly different lifetimes and evolutionary paths huge variation.

18. PHYS 3380 - Astronomy Maximum Masses of Main-Sequence Stars h Carinae (Eta Carinae) a) More massive clouds fragment into smaller pieces during star formation. b) Very massive stars lose mass in strong stellar winds Eddington limit - point where gravitational force can no longer balance the continuum radiation force outwards. Exceeding the Eddington limit - star initiates very intense driven stellar wind from its outer layers. Example: h Carinae: Binary system of a 60 M  and 70 M  star. Dramatic mass loss; major eruption in 1843 created double lobes. M max ~ 100 solar masses

19. The Eddington Limit or Eddington luminosity The point at which the luminosity emitted by a star or active galaxy is so extreme that it starts blowing off the outer layers of the object. i.e., the greatest luminosity that can pass through a gas in hydrostatic equilibrium, meaning that greater luminosities destroy the equilibrium. - named after the British astrophyicist Sir Arthur Stanley Eddington - famous for confirming the general theory of relativity using eclipse observations. - Eddington limit is likely reached around 120 solar masses, at which point a star starts ejecting its envelope through intense solar wind. - Wolf-Rayet stars are massive stars showing Eddington limit effects, ejecting.001% of their mass through solar wind per year.

20. PHYS 3380 - Astronomy Minimum Mass of Main-Sequence Stars M min = 0.08 M  At masses below 0.08 M , stellar progenitors do not get hot enough to ignite thermonuclear fusion.  Brown Dwarfs Gliese 229B

21. PHYS 3380 - Astronomy Brown Dwarfs Hard to find because they are very faint and cool; emit mostly in the infrared. Many have been detected in star forming regions like the Orion Nebula.

22. PHYS 3380 - Astronomy The structure and evolution of a star is determined by the laws of Main Sequence Stars Hydrostatic equilibrium - weight of each layer balanced by pressure Energy transport - energy moves from hot to cool Conservation of mass - total mass = sum of shell masses Conservation of energy - total luminosity = sum of shell energies A star’s mass (and chemical composition) completely determines its properties. Stars initially all line up along the main sequence - in hydrostatic equilibrium - outward pressure of gas balanced by inward weight

23. PHYS 3380 - Astronomy Stellar Model For isolated, static, and spherically symmetric stars – these laws lead to four basic equations to describe structure. All physical quantities depend on the distance from the centre of the star alone. 1) Equation of hydrostatic equilibrium: at each radius, forces due to pressure differences balance gravity 2) Conservation of mass: Total mass equals sum of shell masses - no gaps. 3) Conservation of energy : at each radius, the change in the energy flux = local rate of energy release 4) Equation of energy transport : relation between the energy flux and the local gradient of temperature

24. PHYS 3380 - Astronomy Solving the Equations of Stellar Structure We can derive four differential equations, which govern the structure of stars - provide set of coupled equations for determining stellar model. r = radius  = density at r P = pressure at r M = mass of material within r L = luminosity at r (rate of energy flow across sphere of radius r) T = temperature at r  R = Rosseland mean opacity at r - opacity of gas of given composition, temperature, and density, averaged over the various wavelengths of the radiation being absorbed and scattered.  = energy release per unit mass per unit time P = P ( , T, chemical composition)  R =  R ( , T, chemical composition) -  =  ( , T, chemical composition) These quantities dependent on density, temperature, and chemical composition

25. PHYS 3380 - Astronomy Boundary Conditions Two of the boundary conditions are fairly obvious, at the centre of the star M=0, L=0 at r=0 At the surface of the star its not so clear, but we use approximations to allow solution. There is no sharp edge to the star, but for the the Sun  (surface)~10 -4 kg m -3. Much smaller than mean density  (mean)~1.4  10 3 kg m -3 (which we derived). We know the surface temperature (T eff =5780K) is much smaller than its minimum mean temperature (2  10 6 K). Thus we make two approximations for the surface boundary conditions:  = T = 0 at r=r s i.e. that the star does have a sharp boundary with the surrounding vacuum

26. PHYS 3380 - Astronomy Use of Mass as the Independent Variable The preceding formulae would (in principle) allow theoretical models of stars with a given radius. However from a theoretical point of view it is the mass of the star which is chosen, the stellar structure equations solved, then the radius (and other parameters) are determined. We observe stellar radii to change by orders of magnitude during stellar evolution, whereas mass appears to remain constant. Hence it is much more useful to rewrite the equations in terms of M rather than r. If we divide the other three equations by the equation of mass conservation, and invert the latter: With boundary conditions: r=0, L=0 at M=0  =0, T=0 at M=M s We specify M s and the chemical composition and now have a well defined set of relations to solve. It is possible to do this analytically if simplifying assumptions are made, but in general these need to be solved numerically on a computer.

27. PHYS 3380 - Astronomy The equations are not time dependent - we must iterate with the calculation of changing chemical composition to determine short steps in the lifetime of stars. The crucial changing parameter is the H/He content of the stellar core. Stellar Evolution So we can evolve a model using The set of equations must be supplemented by equations describing the rate of change of abundances of the different chemical elements. Let C X,Y,Z be the chemical composition of stellar material in terms of mass fractions of hydrogen (X), helium, (Y) and metals (Z) [e.g. for solar system X=0.7,Y=0.28,Z=0.02]

28. PHYS 3380 - Astronomy Theoretical Stellar Evolution Model The outcome is a theoretical HR- diagram.

29. PHYS 3380 - Astronomy The Main-Sequence Phase Pressure increases steeply in centre - 50% of mass is within radius 0.25R - only 1% of total mass is in the convection zone and above - no convective process in 99% of star - does not become fully mixed. - core becomes He rich. Fusion is most efficient in the centre, where T is highest.

30. PHYS 3380 - Astronomy Hipparcos satellite measured 10 5 bright stars with  p>0.001"  confident distances for stars with d<100 pc Hertzsprung-Russell diagram for the 41704 single stars from the Hipparcos Catalogue with relative distance precision better than 20% and  (B-V) less than or equal to 0.05 mag. Colors indicate number of stars in a cell of 0.01 mag in (B-V) and 0.05 mag in absolute magnitude (M V ). Notice the spread in stars on main sequence.

31. PHYS 3380 - Astronomy Evolution on the Main Sequence Zero-Age Main Sequence (ZAMS) MS evolution Main-Sequence stars live by fusing H to He. - finite supply of H => finite life time. As star evolves, H consumed, chemical composition changes (H/He ratio). - total number of nuclei becomes less - pressure reduced - gravity - pressure stability unbalanced - core contracts - temperature and density increase and nuclear reaction rate increases - star becomes more luminous - additional energy flowing out forces outer layers to expand and cool Star gradually becomes larger, brighter, and cooler  Slow changes cause star to move up and to the right on HRD - main sequence not a line but a band - Sun about 30% brighter than when at ZAMS

32. PHYS 3380 - Astronomy Lifetime on the Main Sequence Dependent on mass For the few main-sequence stars for which masses are known, there is a Mass-luminosity relation. L  M n Where n=3-5. Slope changes at extremes, less steep for low and high mass stars. This is why the main-sequence on the HRD is a function of mass i.e. from bottom to top of main- sequence, stars increase in mass

33. The mass-luminosity relation flattens out at higher masses, due to the contribution of radiation pressure in the central core. (This helps support the star, and decreases the central temperature slightly.) The relation also flattens significantly at the very faint end of the luminosity function. This is due to the increasing important of convection for stellar structure. Main sequence stars also obey a mass-radius relation. This relation displays a significant break around 1M  ; R /M ξ, with ξ≈0.57 for M > 1M , and ξ≈0.8 for M < 1M . This division marks the onset of a convective envelope. Convection tends to increase the flow of energy out of the star, which causes the star to contract slightly. As a result, stars with convective envelopes lie below the mass-radius relation for non-convective stars and also moves the star above the nominal mass-luminosity relation. The depth of the convective envelope increases with decreasing mass. Stars with M≈1M  have extremely thin convective envelopes, while stars with M < ~0.3M  are entirely convective. Nuclear burning ceases around M≈ 0.08M . The region of nuclear energy generation is restricted to a very small mass range near the center of the star. The rapid fall-off of ε n (energy release per unit mass per unit time) with radius reflects the extreme sensitivity of energy generation to temperature. Stars with masses below ~ 1M  generate most of their energy via the proton-proton chain. Stars with more mass than this create most of their energy via the CNO cycle. This changeover causes a shift in the energy transport in stellar interiors.

34. PHYS 3380 - Astronomy Lifetime on the Main Sequence A star’s life time T ~ energy reservoir / luminosity Energy reservoir ~ M Luminosity: L ~ M 3.5 T ~ M/L ~ 1/M 2.5 Massive stars have short lives. Red dwarfs use fuel so slowly, should survive for 200 - 300 billion years - all still in infancy since age of universe 10 - 20 billion years

35. PHYS 3380 - Astronomy The Source of Stellar Energy In the sun, this happens primarily through the proton-proton (PP) chain Recall from our discussion of the sun: Stars produce energy by nuclear fusion of hydrogen into helium.

36. PHYS 3380 - Astronomy The CNO Cycle In stars slightly more massive than the sun, a more powerful energy generation mechanism than the PP chain takes over: The CNO Cycle. Highly temperature dependent

37. PHYS 3380 - Astronomy Energy Transport Structure Inner radiative, outer convective zone Inner convective, outer radiative zone CNO cycle dominantPP chain dominant

38. PHYS 3380 - Astronomy Summary: Stellar Structure Mass Sun Radiative Core, convective envelope; Energy generation through PP Cycle Convective Core, radiative envelope; Energy generation through CNO Cycle

39. As a result of the extreme temperature dependence of CNO burning, those stars that are dominated by CNO fusion have very large values of L/4πr 2 in the core. This results in convective instability and convective energy transport is extremely efficient. Because of the extreme temperature sensitivity of CNO burning, nuclear reactions in high mass stars are generally confined to a very small region, much smaller than the size of the convective core. - conditions under which a region of a star is unstable to convection is expresses by the Schwarzschild criterion: where g is the gravitational acceleration, and C p is the heat capacity. A parcel of gas that rises slightly will find itself in an environment of lower pressure than the one it came from. As a result, the parcel will expand and cool. If the rising parcel cools to a lower temperature than its new surroundings, so that it has a higher density than the surrounding gas, then its lack of buoyancy will cause it to sink back to where it came from. However, if the temperature gradient is steep enough (i. e. the temperature changes rapidly with distance from the center of the star), or if the gas has a very high heat capacity (i. e. its temperature changes relatively slowly as it expands) then the rising parcel of gas will remain warmer and less dense than its new surroundings even after expanding and cooling. Its buoyancy will then cause it to continue to rise. The region of the star in which this happens is the convection zone.