Understanding Stellar Lifecycle: From Birth to Death and the Impact of Mass on Lifetimes
This overview explores the complex lifecycle of stars, detailing the fundamental processes involved in their formation, stability, and eventual death. We will examine concepts such as the Stefan-Boltzmann Law and hydrostatic equilibrium, and how mass influences luminosity and life expectancy. By analyzing the distances to stars and their energy production rates, we can estimate stellar lifetimes across different mass ranges. The study also includes practical applications in observing star clusters and their implications for understanding stellar evolution in the universe.
Understanding Stellar Lifecycle: From Birth to Death and the Impact of Mass on Lifetimes
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Presentation Transcript
Homework #10 • Cosmic distance ladder III: Use formula and descriptions given in question text • Q7: Luminosity, temperature and area of a star are related by the Stefan-Boltzmann-Law: L = b A T4, so use scaling arguments to figure out L from R,T and R from L,T
Homework #10 • Q9: Estimate life expectancy from energy production rate and available fuel (mass) • Example: Star with 4L and 3M uses 4 times more mass for energy production, but has 3 times more mass, so it life time is a factor ¾=0.75 compared to the sun: 7.5 billion years • Q8: Given are m and M, so use the distance formula d(m,M) from Q5.
The Fundamental Problem in studying the stellar lifecycle • We study the subjects of our research for a tiny fraction of its lifetime • Sun’s life expectancy ~ 10 billion (1010) years • Careful study of the Sun ~ 370 years • We have studied the Sun for only 1/27 millionth of its lifetime!
Suppose we study human beings… • Human life expectancy ~ 75 years • 1/27 millionth of this is about 74 seconds • What can we learn about people when allowed to observe them for no more than 74 seconds?
Theory and Experiment • Theory: • Need a theory for star formation • Need a theory to understand the energy production in stars make prediction how bight stars are when and for how long in their lifetimes • Experiment:observe how many stars are where when and for how long in the Hertzsprung-Russell diagram • Compare prediction and observation
Hydrostatic Equilibrium • Two forces compete: gravity (inward) and energy pressure due to heat generated (outward) • Stars neither shrink nor expand, they are in hydrostatic equilibrium, i.e. the forces are equally strong Heat Gravity Gravity
Star Formation & Lifecycle • Contraction of a cold interstellar cloud • Cloud contracts/warms, begins radiating; almost all radiated energy escapes • Cloud becomes dense opaque to radiation radiated energy trapped core heats up
Example: Orion Nebula • Orion Nebula is a place where stars are being born
Protostellar Evolution • increasing temperature at core slows contraction • Luminosity about 1000 times that of the sun • Duration ~ 1 million years • Temperature ~ 1 million K at core, 3,000 K at surface • Still too cool for nuclear fusion! • Size ~ orbit of Mercury
Path in the Hertzsprung-Russell Diagram Gas cloud becomes smaller, flatter, denser, hotter Star
Protostellar Evolution • increasing temperature at core slows contraction • Luminosity about 1000 times that of the sun • Duration ~ 1 million years • Temperature ~ 1 million K at core, 3,000 K at surface • Still too cool for nuclear fusion! • Size ~ orbit of Mercury
Path in the Hertzsprung-Russell Diagram Gas cloud becomes smaller, flatter, denser, hotter Star
A Newborn Star • Main-sequence star; pressure from nuclear fusion and gravity are in balance • Duration ~ 10 billion years (much longer than all other stages combined) • Temperature ~ 15 million K at core, 6000 K at surface • Size ~ Sun
Mass Matters • Larger masses • higher surface temperatures • higher luminosities • take less time to form • have shorter main sequence lifetimes • Smaller masses • lower surface temperatures • lower luminosities • take longer to form • have longer main sequence lifetimes
Mass and the Main Sequence • The position of a star in the main sequence is determined by its mass All we need to know to predict luminosity and temperature! • Both radius and luminosity increase with mass
Stellar Lifetimes • From the luminosity, we can determine the rate of energy release, and thus rate of fuel consumption • Given the mass (amount of fuel to burn) we can obtain the lifetime • Large hot blue stars: ~ 20 million years • The Sun: 10 billion years • Small cool red dwarfs: trillions of years The hotter, the shorter the life!
Main Sequence Lifetimes Mass(in solar masses)LuminosityLifetime 10 Suns 10,000 Suns 10 Million yrs 4 Suns 100 Suns 2 Billion yrs 1 Sun 1 Sun 10 Billion yrs ½ Sun 0.01 Sun 500 Billion yrs
Is the theory correct? Two Clues from two Types of Star Clusters Open Cluster Globular Cluster
Star Clusters • Group of stars formed from fragments of the same collapsing cloud • Same age and composition; only mass distinguishes them • Two Types: • Open clusters (young birth of stars) • Globular clusters (old death of stars)
What do Open Clusters tell us? • Hypothesis: Many stars are being born from a interstellar gas cloud at the same time • Evidence: We see • “associations” of stars • of same age • Open Clusters
Why Do Stars Leave the Main Sequence? • Running out of fuel
Stage 8: Hydrogen Shell Burning • Cooler core imbalance between pressure and gravity core shrinks • hydrogen shell generates energy too fast outer layers heat up star expands • Luminosity increases • Duration ~ 100 million years • Size ~ several Suns
Stage 9: The Red Giant Stage • Luminosity huge (~ 100 Suns) • Surface Temperature lower • Core Temperature higher • Size ~ 70 Suns (orbit of Mercury)
Lifecycle • Lifecycle of a main sequence G star • Most time is spent on the main-sequence (normal star)
The Helium Flash and Stage 10 • The core becomes hot and dense enough to overcome the barrier to fusing helium into carbon • Initial explosion followed by steady (but rapid) fusion of helium into carbon • Lasts: 50 million years • Temperature: 200 million K (core) to 5000 K (surface) • Size ~ 10 the Sun
Stage 11 • Helium burning continues • Carbon “ash” at the core forms, and the star becomes a Red Supergiant • Duration: 10 thousand years • Central Temperature: 250 million K • Size > orbit of Mars
Deep Sky Objects: Globular Clusters • Classic example: Great Hercules Cluster (M13) • Spherical clusters • may contain millions of stars • Old stars • Great tool to study stellar life cycle
Observing Stellar Evolution by studying Globular Cluster HR diagrams • Plot stars in globular clusters in Hertzsprung-Russell diagram • Different clusters have different age • Observe stellar evolution by looking at stars of same age but different mass • Deduce age of cluster by noticing which stars have left main sequence already
Catching Stellar Evolution “red-handed” Main-sequence turnoff
Type of Death depends on Mass • Light stars like the Sun end up as White Dwarfs • Massive stars (more than 8 solar masses) end up as Neutron Stars • Very massive stars (more than 25 solar masses) end up as Black Holes
Reason for Death depends on Mass • Light stars blow out their outer layers to form a Planetary Nebula • The core of a massive star (more than 8 solar masses) collapses, triggering the explosion of a Supernova • Also the core of a very massive stars (more than 25 solar masses) collapses, triggering the explosion Supernova
Light Stars: Stage 12 - A Planetary Nebula forms • Inner carbon core becomes “dead” – it is out of fuel • Some helium and carbon burning continues in outer shells • The outer envelope of the star becomes cool and opaque • solar radiation pushes it outward from the star • A planetary nebula is formed Duration: 100,000 years Central Temperature: 300 106 K Surface Temperature: 100,000 K Size: 0.1 Sun
Deep Sky Objects: Planetary Nebulae • Classic Example: Ring nebula in Lyra (M57) • Remains of a dead, • exploded star • We see gas expanding in a sphere • In the middle is the dead star, a “White Dwarf”
Stage 13: White Dwarf • Core radiates only by stored heat, not by nuclear reactions • core continues to cool and contract • Size ~ Earth • Density: a million times that of Earth – 1 cubic cm has 1000 kg of mass!
Stage 14: Black Dwarf • Impossible to see in a telescope • About the size of Earth • Temperature very low almost no radiation black!