ASTR-101 4/4/2018 Stellar Evolution: Part II Lecture...
Transcript of ASTR-101 4/4/2018 Stellar Evolution: Part II Lecture...
ASTR-1014/4/2018
Stellar Evolution:Part II
Lecture 19
WHEN’S THE NEXT TEST ?!?!?!?
• If anyone is following the syllabus, you know that it says there is a test today.
• The test will be on April 11th (a week from today)
• Topics will include:• The Sun
• Measuring the Stars
• Interstellar medium
• Star Evolution
• Star Death
• Obstacle course for extra credit-any injures will result in F
Possible Extra Credit Option
• Kinematics of Parsec-scale Jets of Gamma-Ray Blazars and Connection between Jet events and Gamma-Ray activity 2:00 pm, Thursday, Room 190, Physics & Astronomy
• Please let me know if you are going so that I can attend as well.• Summarize:
• What is the goal of the presented research• Describe the experimental setup• What issues they are encountered• What are the results.
• At least a half a page• Points will be awarded based on completeness and at my discretion.• Up to 5% of a single test grade
More Massive Stars
Quantum Degeneracy Pressure
• Quantum mechanics states that particles (electron, protons, and neutrons) exist in discrete states.
• If all possible states for a given system are filled, no more particles can be added.
• The result is an emergent pressure against compression of matter into smaller volumes of space.
• This is the pressure that holds together a White Dwarf:• White Dwarfs are in hydrostatic equilibrium
• White Dwarfs have no fusion
• With quantum degeneracy pressure, gravity would crush the star
• If the Main-Sequence binary companion is close enough, the white dwarf is able to ‘steal’ the upper layers from its companion.
• As the hydrogen envelope is accreted onto the white dwarf, fusing begins and the accretion disk is quickly ignited.
• This process can happen many times, depending on the mass of the companion star.
Novae
Type1a Supernovae
• As the hydrogen envelope is accreted onto the white dwarf, fusing begins and the accretion disk is quickly ignited.
• This process can happen many times, but eventually comes to a stop once the mass becomes large enough.
• If the mass gets above the Chandrasekhar limit, 1.4 solar masses, the star cannot support the force of gravity.
• The star suddenly fusses all the carbon at once.
Type II supernovae-Core Collapse Super Novae
• Hydrostatic equilibrium is lost because Iron does not burn.
• Before this point core was held up by electron degeneracy pressure and nuclear fusion.
• Core is compressed, due to gravity, by overlying layers.
• Electron degeneracy pressure is not strong enough and the core collapses, compressing objects even further.
• Photodisintegration occurs and many neutrons are created as heavy nuclei are ripped apart.
• Neutrons get squeezed inside of the core.
• Collapsing star is halted by neutron degeneracy pressure, resulting in a violent, fast, rebound of the collapsing material.
Death of Massive Starts
• Stars with a mass greater than 8 solar masses will end their lives in a massive explosion called a core collapse supernova.
• This happens when the core starts to fuse Silicon in Iron.
• Unlike lighter elements, fusing Iron into heavier elements does not produce energy. It takes energy away from the system.
Core-burning nuclear fusion stages for a 25-solar mass star
ProcessMain fuel
Main products
25 M☉ star
TemperatureDuration
(K)
hydrogen burning hydrogen helium 7×107 107 years
triple-alpha process
heliumcarbon,oxygen
2×108 106 years
carbon burning process
carbonNe, Na, Mg, Al
8×108 103 years
neon burning process
neon O, Mg 1.6×109 3 years
oxygen burning process
oxygen Si, S, Ar, Ca 1.8×109 3.5 months
silicon burning process
silicon iron 2.5×109 5 days
Star Clusters
• Stars that form in the same molecular cloud have very similar initial conditions.
• Groups of stars gravitationally bound are called star clusters.
• Often they are moving around a common central point.
• Stars will differ in mass, but be compositionally the same.
• Massive stars evolve fast.
• Low mass stars evolve slow.
16,000 light-years away, Omega Centauri, most massive globular cluster
Globular Clusters • nearly symmetrical round systems of, typically, hundreds of thousands of stars.
• Globular clusters are the oldest part of our Milky Way.
• If Earth orbited one of the inner stars in a globular cluster, the nearest stars would be light-months, not light-years, away.
• Found mostly in the Halo of our galaxy.
Open Cluster• Open clusters contain up to a
few hundred stars and are not much older than our Sun.
• The youngest open clusters are still associated with the interstellar matter from which they formed. 30 light year diameter
• The average speed of the member stars may be higher than the cluster’s escape velocity,
• The stars will gradually “evaporate” from the cluster
Stellar Association• Stellar Associated stars are a
group of less than 50 hot bright young stars scattered over 100-500 light year diameter.
• the constellation Orion is an example.
• Also contains many low mass proto-stars.
• Always shrouded in dense ISM.
Main Sequence Turnoff
• Once a star stops burning hydrogen, it will turn off of the main sequence.
• The more massive the star the quicker it will make this turn.
• What population is still left on the Main Sequence dictates the age of the cluster.
• Open clusters turn out to be as young as 1 to a few 100 million years old.
• Globular clusters have main sequence stars that turn off at a luminosity less than that of the Sun (10 billions years)
What type of cluster is this?
Heavy Metals in Clusters
• Like our Sun, open clusters contain 1-4% metals (things heavier than hydrogen and helium).
• Globular clusters contain much less heavy metals (< 1%).
• Heavy elements are created from star death, which enriches the ISM.
• The first generation of stars were only hydrogen and helium because not enough time had pasted for stars to die.
• This means that the first generation of stars that formed in our Galaxy would not have been accompanied by a planet like Earth
• Gaia, launched by ESA, has been measuring the position and distances to almost one billion stars with an accuracy of a few tenmillionths of an arcsecond.
• Giving us a three-dimensional map of a large fraction of our own Milky Way Galaxy.
• These precision measurements help improve the distances measurement techniques using the H-R diagram.
Using Parallax to map out the Milky Way
Roughly ~30,000 parsecs
Variable Stars• Recall that the apparent brightness of an object decreases with the
square of the distance to that object.
• A light curve represents how bright a star is as a function of time
• What would the light curve of our Sun look like?
Pulsating Variable Stars
• Cepheid and RR Lyrae variables are pulsating variable stars, meaning they change diameter as a function of time.
• The expansion and contraction can be measured using Doppler shift.
• This physical phenomenon happens during the brief Red Giant phase of some more massive stars.
• As the star expands, it cools.
• Once it becomes cool enough, it contracts (gravity dominates pressures).
The Period-Luminosity Relation
• Cepheid have a very consistent period of luminosity fluctuation occurring between 3-50 days.
• Because they are in the red giant phase, they are 1000-10,000 times brighter than the Sun (easy to spot).
• The amazing part: The brighter the star, the longer the period.
• Measuring the period of the fluctuations gives the intrinsic brightness of the star.
• By comparing absolute brightness and relative brightness measured on Earth and using the inverse square law, an distance can be measured!
Henrietta Leavitt
• Leavitt discovered hundreds of variable stars in the Large MagellanicCloud and Small Magellanic Cloud.
• She concluded that all variable stars in these galaxies were at about the same distance.
• Any difference in their apparent brightnesses must be caused by differences in their intrinsic luminosities.
• Leavitt found that brighter stars have longer periods and concluded that their period must be related to the absolute brightness of the star.
Type1a Supernovae
• Type1a supernovae always explode at 1.4 solar masses -> always have the same brightness.
• Crucially they also have an easily identified light curve.
• Using Cephied variable stars to measure the distance to supernovae, astronomers can use typ1a supernovae light curves to measure distances.