Title: Chapter 5: Cosmic foundations for origins of life stars
1 Chapter 5 Cosmic foundations for
origins of life - stars
2Stellar evolution forming the elements for
biolmolecules and planets.
- Stars are fusion reactors that convert lighter
elements into heavier ones, liberating energy
(from Emc2) - They therefore continuously evolve as their
fuels are used up. H burns to He, He burns to C,
etc - Stellar end-states white dwarfs, neutron
stars, or black holes. - In all of these cases, significant fraction of
stellar mass, ejected into interstellar medium - Planets, and biomolecules made out of these
materials
3Energy liberated when light atomic nuclei undergo
fusion! (eg. Proton-proton reaction)
- Two protons colliding at high enough speed,
undergo fusion. - Products a deuteron (heavy water), a positron
(positively charged electron), and a neutrino
(very weakly interacting particle) energy
release - Special Relativity Energy release per fusion
is proportional to mass difference between
products and reactants
4 Energy production in the Suns core
the proton-proton chain
5 Net result of p-p burn
- For each Helium-4 nucleus produced
- - Consume 4 protons
- - Liberate energy and 2 neutrinos
- - Neutrinos arise from weak interaction.
- eg. they arise during conversion of a proton
to a neutron in building a deuteron - Nuclear reactions yield predictable neutrino
fluxes from the Sun that directly reflect
reaction rates
6Stellar temperatures
- Stars have different colours
- Corresponds to different temperatures from black
body curves - Note huge (and harmful) UV fluxes produced by
massive stars - (life possible on planets around them?)
7Spectral Classification of Stars Consequence
ofstellar temperatures
- - Stellar spectra can be divided into spectral
classes of stars O,B,A,F,G,K,M - Atomic theory this represents a sequence of
decreasing temperature - hot stars are more
completely ionized than cool stars so see fewer
absorption features. - - The Sun is a G2 star.
8Hertzsprung-Russell Diagram Plotting L vs. T
- Luminosity L and temperature T of a star are
independent physical properties of a star. - Temperature correlates with colour of a star (hot
is blue, cool is red). L varies by factor of 100
million! - Plot L of a star vs. its colour on a diagram
find that these are correlated with one another.
Known as colour-magnitude diagram. - - Most stars occur along main-sequence, where
they burn hydrogen.
9H-R Diagrams (L vs. T) of Nearest, and brightest
stars
Stars within 5pc of Sun
100 brightest stars in the sky
10- STELLAR RADII
- Range from 0.08 of the Sun, to 630 times the
Suns radius (Betelgeuse) - Giants radii of 10 100 solar radius
- (Mira is Red Giant)
- Supergiants up to 1000 solar radii
11- Main Sequence Stars confined to well defined
band from top left (high T, high L), to bottom
right (low T, low L). - Temperature range over main sequence 3,000K (M
type) 30,000 K (O type) 1 decade in
temperature - Range in luminosities over 8 decades!
- - partly explained by black body relation
- At top end stars are hot and large blue
supergiants - At bottom end stars are cool and small red
dwarfs - O and B stars extremely rare one in 10,000
- Stars spend most of their life on main-sequence
burning hydrogen
12- Off the main sequence
- Red giants (upper right of H-R diagram high L,
low T) and white dwarfs (lower left low L,
high T). - Red giants burn hydrogen in a shell
- White dwarfs hard to detect very faint
- Sun will go through red-giant phase and end up as
a cooling white dwarf. - Red giant will swell to orbit beyond Earth
consequences for life!
13Main sequence is a mass sequence ie stellar mass
determines stellar properties
14Structure of Red Giant star furious hydrogen
burning occurs in a shell gradually moving out
through unburned material. Non-burning He ash
accumulates in core.
After 10 billion years, core of solar mass star
uses up H, and consists of He. Fusion ceases at
centre of core, and it begins to contract. Star
leaves main sequence.
15Red Giant Branch
- Subgiant Branch Stage 7 Stage 8
- H burns in a shell, He ash accumulates in core.
- Red Giant Branch Stage 8 stage 9
- - Outer layers of star so cool that convection
throughout star occurs so ascend a vertical
track
16- Tip of Giant Branch
- Radius is 100 solar radii (size of Mercurys
orbit) - He core is 1/1000 size of star - few times
larger than the Earth. 25 of stellar mass locked
up in core - 10,000 times the luminosity of the Sun.
- Core density, about 100 million kg/ cubic metre.
- Envelope density, about 1/1000 kg/ cubic metre
17Helium fusion the Triple-Alpha Process
fine tuning!
- At stage 9 tip of Giant Branch central
temperatures are - 100 million K, at densities of
kg/cubic metre, conditions allow ignition of
helium ash accumulating in stellar core - Beryllium 8 highly unstable. Decays very
quickly into 2 alpha particles again - about
! SLIGHT CHANGE IN STRENGTH OF
NUCLEAR FORCE AND THIS REACTION IS IMPOSSIBLE! - Resonant interaction between Be and alpha
particle allow second reaction above to occur -
carbon is the ash
18Horizontal Branch Helium Main-Sequence
- Helium Flash Explosive onset of He burning at
tip of Red Giant Branch (RGB). (stage 9) - He burning core (stage 10) known as Horizontal
Branch.
19Ascending the Asymptotic Giant Branch the
Accumulation of Carbon
- When He in core of star on Horizontal Branch is
used up He shell burn commences star moves
off Horizontal Branch. - Now have 2 burning shells, H, and deeper in, He
with Carbon ash accumulating in core - Star moves up asymptotic giant branch
increasing in size and luminosity. Carbon core
continues to contract
20- Horizontal Branch (stage 10) He core burn
and H shell burn. The Main-Sequence for He
burning. - Asymptotic Giant Branch (AGB) stage 10 stage
11 Shell burning for both He and H. Carbon
ash accumulates in core. - Produces much larger red star Red Supergiant
500 solar radii swallows Mars!, surface
temperature 4000 K, central T 250 million K.
215 billion years into the future the fate of the
Sun
- Planetary nebula NGC 3132.
- - ejection of envelope of star leaving a
degenerate stellar core (white dwarf). - White dwarf
- Outer edge of envelope
22Evolution of Massive Stars
- Stars more massive than 8 solar masses lead to
supernova explosions - High mass stars move almost horizontally (rather
than vertically) in post main-sequence evolution - - luminosity of star stays fairly constant but
radius increases,reducing surface temperature - High mass stars fuse carbon, oxygen, and other
elements
23- For massive stars (more than 8 solar masses)
series of burning shells ash of burn above it
igniting producing ash beneath it. - Creates an onion-like series of burning
layers. at bottom of which is iron ash. - Carbon burns for 1000 yr, oxygen for a yr,
silicon for a week. - Iron core grows for less than a day!
24Iron is natures most stable element
- Small nuclei liberate energy by fusion
- Elements more massive than iron liberate energy
by fission into smaller nuclei. - IRON DOES NOT BURN!
- Degenerate iron core is end-state of nuclear
fusion in interior.
25Carbon burning (a) occurs at T 600 million K,
while (b) occurs at 200 million K
26The route to iron
Oxygen Fusion
Silicon Burning Building up to Nickel (T 3
billion K !)
Nickel-56 quickly decays via cobalt-56 into
stable iron-56
27Synthesizing Elements Beyond Iron
- Occurs by neutron capture to iron (which just
changes the isotope), followed by radioactive
decay into stable element eg. - Neutron capture occurs during supernova explosion
(high density and temperature) either by
rapid (r) or slow (s) process - Elements produced during explosion much rarer
because time available to produce them is so
short
28Nucleosynthesis in stars explains abundances of
the elements
- Sharp drop in abundance as go to higher atomic
number reflects increasing Coulomb barrier to
fusion - Peaks and troughs in distribution reflect
stable closed shell nuclei, etc.
29Supernova remnant the Crab nebula (supernova
seen by Chinese astronomers in 1054 A.D.)
30Canadian Galactic Plane Survey (CGPS) the
interstellar medium stirred by supernova
explosions and stellar winds.Map of atomic
hydrogen. Midplane of Milky Way - near
constellation Perseus