Stellar Evolutiona

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Transcript Stellar Evolutiona

Stellar Evolution

Andrej Ficnar & Lovro Prepolec 5 th April 2005

Introduction

    A star is any massive gaseous body in space About 70×10

21

known universe stars in Lifetime from millions to billions of years Origins of chemical

elements

Introduction

  Aging and death of stars lead to many interesting astronomical phenomena:  Black holes  Neutron stars  Dwarves  Nebulas First scientific theories in 19th century (Kelvin and Helmholtz)

Formation of Stars

    Form from interstellar gas

clouds Gravitational

collapse of gas clumps Flattening of clumps Formation of a

protostar

Formation of Stars

Formation of Stars

   Protostars - cold and have short lifetime Characterized by

outflow of gas

Mass of most stars between about 0.1 and 30 M

S

Main Sequence Stars

   Characterized by

hydrostatic equilibrium

Name from

Hertzsprung Russel diagram

Main - sequence lifetime approx.: where M and L are mass and luminosity in solar units

Leaving the Main Sequence

  Main sequence star eventually becomes red

giant

Star switches to helium burning by compressing the core

Low - Mass Stars

 Mass < 10 M

S

, colder, less luminous, longer lifetime  To start helium burning, gas degeneratesHelium flashes transform star into a yellow

giant

 Yellow giants may pulsate  Increased “fuel” consumption leads to red

supergiant

Low - Mass Stars

 Ejection of outer layers forms planetary

nebulas

 Core becomes a white

dwarf

Low - Mass Stars

High - Mass Stars

  Mass > 10 M

S

, hotter, more luminous, shorter lifetime Begin as blue main sequence stars, and afterwards become yellow supergiants     No degeneration or helium flashes No planetary nebulas or white dwarves Different hydrogen fusion process (CNO cycle) Ability of nucleosynthesis

High - Mass Stars

Core of iron shrinks into a core of neutronsGravitational collapse of core leads to explosion –

supernova

 Supernova remnants  Core becomes a neutron star or a black hole

High - Mass Stars

Stellar Remnants: White Dwarves

  Remnants of low-mass stars Shell ejected into planetary nebula       Hot (~ 25 000 K), compact stars Mass comparable to M

S

, but radius comparable to

radius of Earth

Very dim, no fuel burning Cool rapidly (black dwarf) Composed of C and O, surface layer of H and He Extreme magnetic fields (~1000 T)

Stellar Remnants: White Dwarves

Pauli exclusion principle  Very dense packing causes degeneration: added mass causes shrinking  White dwarf may finally collapse  1931 S. Chandrasekhar calculated limiting mass of a white dwarf 

Chandrasekhar limit ~ 1.4 M S

Stellar Remnants: White Dwarves in Binary Systems

Stellar Remnants: Neutron Star

 1934 W. Baade and F. Zwicky   Theoretical results:  Radius ~10 km  Maximum mass ~2 – 3 M S 1967 A. Hewish et al. detected radio signal with astonishingly precise pulse rate  (period of pulsation) ~(density) -1  Densities larger then those of white dwarves

Stellar Remnants: Neutron Star

F. Pacini and T. Gold: pulsar is rotating, not pulsating star   T S ~1 month T pulsar from 1 ms to 4 s Law of conservation of angular momentum  Mechanism of radiation (synchrotron radiation)  X-ray binaries  1974. J. Taylor and R. Hulse: binary pulsar

Stellar Remnants: Black Holes

  Remnants of high-mass stars Escape velocity    1783. J. Michell

P. S. Laplace

K. Schwartzshild, Schwartzshild radius

Stellar Remnants: Black Holes

   Strange properties of black holes   Temperature (J. Bekenstein) (~6×10

-8

K) Radiation (S. Hawking) ( l max ~16 R S ) Gravitational waves Detecting black hole:

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