* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Stellar Evolution
Space Interferometry Mission wikipedia , lookup
Formation and evolution of the Solar System wikipedia , lookup
Aries (constellation) wikipedia , lookup
Constellation wikipedia , lookup
Rare Earth hypothesis wikipedia , lookup
Star of Bethlehem wikipedia , lookup
Canis Minor wikipedia , lookup
Dyson sphere wikipedia , lookup
Corona Borealis wikipedia , lookup
International Ultraviolet Explorer wikipedia , lookup
Corona Australis wikipedia , lookup
Auriga (constellation) wikipedia , lookup
Cassiopeia (constellation) wikipedia , lookup
Observational astronomy wikipedia , lookup
Canis Major wikipedia , lookup
Cygnus (constellation) wikipedia , lookup
Star catalogue wikipedia , lookup
Cosmic distance ladder wikipedia , lookup
Type II supernova wikipedia , lookup
Aquarius (constellation) wikipedia , lookup
Future of an expanding universe wikipedia , lookup
H II region wikipedia , lookup
Timeline of astronomy wikipedia , lookup
Perseus (constellation) wikipedia , lookup
Stellar classification wikipedia , lookup
Open cluster wikipedia , lookup
Stellar kinematics wikipedia , lookup
Corvus (constellation) wikipedia , lookup
Hayashi track wikipedia , lookup
ASTR 1120 Questions: • What does the Hertzprung-Russell diagram mean? • How do stars form? Chapter 16 & start of Chapter 17: `Star Stuff’ Phil Armitage, standing in today for Andrew Hamilton ASTR 1120: Fall 2005 luminosity of the star What properties can we measure for stars? (1) color - recall this tells us about the temperature at the surface of the star (2) how bright the star appears to us temperature If we know the distance (hard!) we can convert the apparent brightness to a luminosity (power in watts) and plot luminosity vs temperature for a collection of stars ASTR 1120: Fall 2005 Ejnar Hertzprung Henry Russell ASTR 1120: Spring 2005 luminosity Giant and supergiant stars Main sequence Dead stars, white dwarfs increasing surface temperature ASTR 1120: Spring 2005 Clicker Q: suppose you observe a binary star where the 2 stars (assume they are identical) are too close to resolve in the telescope (they appear as a single point of light). Where does the binary appear: A: on the main sequence B: above the main sequence C: below the main sequence D: as a supergiant ASTR 1120: Spring 2005 Clicker Q: suppose you observe a binary star where the 2 stars (assume they are identical) are too close to resolve in the telescope (they appear as a single point of light). Where does the binary appear: A: on the main sequence B: above the main sequence C: below the main sequence D: as a supergiant ASTR 1120: Spring 2005 Small amount above the main sequence: - twice as much light (luminosity) from the 2 stars -same color (since the stars are the same) ASTR 1120: Fall 2005 What does the HR diagram represent? 1) An evolutionary sequence - perhaps stars start out hot and bright and become cool and dim, moving along the main sequence as they go? 2) A sequence of stars of different mass each mass star has `its place’ in the diagram and remains there throughout its (mainsequence) life? ASTR 1120: Fall 2005 Almost always, stars evolve very slowly, so even if stars did move along the main sequence we wouldn’t observe that Very beautiful exception - Eta Carina ASTR 1120: Fall 2005 Debate was resolved by measuring the masses of stars at different points along the main sequence Even harder than measuring distances, get mass from motion in binary star systems e.g. the binary Sirius A/B ASTR 1120: Fall 2005 Main sequence Understand the main sequence as stars of different masses fusing hydrogen into helium Higher mass - larger inward force of gravity gravity pressure gradient To balance this, need large central pressure - high central temperature High T means faster nuclear reactions, generating more luminosity ASTR 1120: Spring 2005 luminosity With higher mass, the surface temperature increases and the luminosity increases rapidly increasing surface temperature Roughly, the luminosity of a main sequence star scales as the fourth power of the mass: LµM 4 ASTR 1120: Spring 2005 Main sequence lifetime More massive stars have larger reservoir of fuel (hydrogen) for nuclear fusion BUT they burn it much much faster Massive stars have shorter lives than low mass stars Quantitatively: Fuel µ Mass Luminosity µ Mass 4 Fuel supply 1 Lifetime µ µ 3 Luminosity M e.g. a 2 Solar mass star lives for roughly 1 / 23 (one eighth) as long as the Sun † † ASTR 1120: Spring 2005 Main sequence lifetime Some numbers from computer models of stellar evolution: 0.25 Solar masses: 1000 billion (a trillion!) years 1 Solar mass: 10 billion years 10 Solar masses: 10 million years Short lifetimes of massive stars are crucial to the existence of the Earth - allow products of nuclear burning to be recycled into the Galaxy and form new generations of stars ASTR 1120: Spring 2005 Star clusters Observational clues to what happens at the end of stars’ main sequence lives come from star clusters Most stars form in such clusters - e.g. in the Orion nebula ASTR 1120: Spring 2005 Star formation: a large cloud of gas (thousands of Solar masses) collapses under gravity to form a star cluster ASTR 1120: Spring 2005 Star clusters come in 2 types: Open clusters Modest groupings of stars - up to several thousand Example: the Pleiades cluster in Taurus ASTR 1120: Spring 2005 Star clusters come in 2 types: Globular clusters Can contain a million stars in a region ~100 light years across In our galaxy, globular clusters are all old, whereas new open clusters are being formed now ASTR 1120: Spring 2005 Why clusters are important For both open and globular clusters: • all the stars are at about the same distance from the Earth • all the stars formed at about the same time Determining the distance and age to a globular cluster is much easier than trying to find the distances and ages of a million random stars! Laboratories for understanding how stars of different masses evolve ASTR 1120: Spring 2005 What happens when a star, fusing hydrogen into helium on the main sequence, exhausts the hydrogen in the core? • hydrogen burning stops, star loses energy • core contracts, and gets hotter • higher temperature allows new nuclear reactions to start that are very slow at the ~15 million K temperature maintained by hydrogen fusion Star leaves the main sequence, becomes a red giant! ASTR 1120: Fall 2005 In a H-R diagram star: luminosity - moves to the right - i.e. a lower surface T and a redder color - moves upward, to much higher luminosity increasing surface temperature ASTR 1120: Spring 2005 Atmospheres of the largest giants can (just) be resolved with HST ASTR 1120: Spring 2005 Can date a star cluster by looking for the most massive star that is still on the main sequence: Young Old ASTR 1120: Fall 2005 Point where stars are leaving the main sequence is called main sequence turnoff, it moves to cooler (lower mass) stars with age ASTR 1120: Fall 2005