Upload
sawhney-baldeep-singh
View
259
Download
1
Embed Size (px)
Citation preview
8/3/2019 E5 Stellar Processes and Stellar Evolution
1/29
E5 stellar processes and stellar
evolution (HL only)
8/3/2019 E5 Stellar Processes and Stellar Evolution
2/29
Star formation
8/3/2019 E5 Stellar Processes and Stellar Evolution
3/29
Star formation
Interstellar space consists of gas (74% H, 25% He
by mass) and dust at a density of about 10-21
kg.m-3. This is about one hydrogen atom to every
cm3 of space.
8/3/2019 E5 Stellar Processes and Stellar Evolution
4/29
Star formation
When the gravitational energy of a given mass of
gas exceeds the average kinetic energy of the
molescules the gas cloud becomes unstable and
starts to collapse.
GM2/R > (3/2)NkT
Jeans criterion
8/3/2019 E5 Stellar Processes and Stellar Evolution
5/29
Star formation
As the cloud collapses, the particles get faster
and eventually clumps form that are hot enough
to emit light. Protostars are formed.
8/3/2019 E5 Stellar Processes and Stellar Evolution
6/29
Star formation
If the star is big enough the collapse will
continue until the star is hot enough for nuclear
fusion to occur. The radiation pressure produced
by the fusion balances the pull of gravity and
equilibrium is reached. The star is a main
sequence star (like our sun).
8/3/2019 E5 Stellar Processes and Stellar Evolution
7/29
8/3/2019 E5 Stellar Processes and Stellar Evolution
8/29
Main sequence
41H 4He + 2e+ + 2 + 2e (26.7 MeV)
8/3/2019 E5 Stellar Processes and Stellar Evolution
9/29
Mass v luminosity relation
L Mwhere 3 < > 4
8/3/2019 E5 Stellar Processes and Stellar Evolution
10/29
Mass v luminosity relation
Since the luminosity could be the total energy
given out by the star (E) divided by the
lifetime of the star T we get
E/T M
Since E = Mc2 from Einsteins formula
Mc2
/T M
T M1-
Taking = 4 we get T M-3
8/3/2019 E5 Stellar Processes and Stellar Evolution
11/29
Lifetime of a star
T M-3The bigger the mass of a star, the shorter
its life (it burns out quicker)
A star with a mass 10x greater than the sun will
have a life time a factor 10-3 (1/1000) less than
the sun
8/3/2019 E5 Stellar Processes and Stellar Evolution
12/29
When the hydrogen runs out?
8/3/2019 E5 Stellar Processes and Stellar Evolution
13/29
Schnberg Chandrasekhar limit
After the star has used up about 12% of its
hydrogen, its core will contract but the outer
layers will expand substantially ()fusion
continues there). The star leaves the main
sequence and moves over to the Red Giant
branch
8/3/2019 E5 Stellar Processes and Stellar Evolution
14/29
Mstar < 0.25Msun
No further nuclear reactions
Core stays as Helium
After a Red giant it becomes a White Dwarf
8/3/2019 E5 Stellar Processes and Stellar Evolution
15/29
0.25Msun < Mstar < 4Msun
Core temperature reaches 108 K enabling
Helium fusion (higher temperature is needed
because Helium nuclei have 2 positive
charges)
Helium fuses to form oxygen and carbon
After a Red gaint a White Dwarf with a
carbon/oxygen core is formed
8/3/2019 E5 Stellar Processes and Stellar Evolution
16/29
4Msun < Mstar < 8Msun
Core temperature rises further enabling the
fusion of carbon and oxygen to take place
producing a core of oxygen, neon and
magnesium
After a Red giant a White Dwarf with an
oxygen/neon/magnesium core is formed
8/3/2019 E5 Stellar Processes and Stellar Evolution
17/29
8Msun < Mstar
Core temperature rises further so heavier
elements fuse. Helium in the outer layers
continues to fuse too. Eventually iron is
produced (which does not fuse see topic 7)
This is a RED SUPERGIANT
Will eventually become a NEUTRON STAR
8/3/2019 E5 Stellar Processes and Stellar Evolution
18/29
Anatomy of a RED SUPERGIANT
and neon
8/3/2019 E5 Stellar Processes and Stellar Evolution
19/29
Evolution of stars < 8Msun
Core contracts under its own weight
It stops when electrons have to be forced into
the same quantum state. This is not allowedso this electron degeneracy pressure stops
the star collapsing further
The outer layers are released to form a
planetary nebula
The resultant White dwarfhas no energy
source so is doomed to cool down to become
a Black dwarf.
8/3/2019 E5 Stellar Processes and Stellar Evolution
20/29
Evolution of stars > 8Msun
If the core is above 1.4 solar masses (the
Chandrasekhar limit) Electrons are forced into
protons producing neutrons.
The core is only made of neutrons and
contracting rapidly.
8/3/2019 E5 Stellar Processes and Stellar Evolution
21/29
Evolution of stars > 8Msun
The neutrons get too close to each other (this
time it is neutron degeneracy pressure
caused by neutrons not being allowed to
occupy the same quantum state) and the
entire core rebounds to a larger equilibrium
size.
The causes a catastophic shock wave whichexplodes the star in a SUPERNOVA
8/3/2019 E5 Stellar Processes and Stellar Evolution
22/29
Evolution of stars > 8Msun
The neutron star left over after the supernova
remains stable provided its has a mass of no
more than 3 solar masses (the Oppenheimer-
Volkoff limit)
8/3/2019 E5 Stellar Processes and Stellar Evolution
23/29
Evolution of stars > 8Msun
Neutron stars with masses substantially more
than the Oppenheimer-Volkoff limit continue
to collapse as the neutron pressure is
insufficient. They become Black holes
At the centre of the black hole is a singularity
The boundary around the singularity where
even light does not have sufficient escape
velocity to escape is called the event horizon
or gravitational radius.
8/3/2019 E5 Stellar Processes and Stellar Evolution
24/29
Stellar evolution
8/3/2019 E5 Stellar Processes and Stellar Evolution
25/29
Evolution of stars on the HR diagram
8/3/2019 E5 Stellar Processes and Stellar Evolution
26/29
8/3/2019 E5 Stellar Processes and Stellar Evolution
27/29
Evolution of stars on the HR diagram
8/3/2019 E5 Stellar Processes and Stellar Evolution
28/29
Pulsars Another very important property of neutron star is
its strong magnetic field. When electrons move in
spirals around magnetic lines of force, radio waves
are produced and radiated out along the two
magnetic poles of the star.
8/3/2019 E5 Stellar Processes and Stellar Evolution
29/29
Pulsars Usually, the rotational axis of the neutron star does
not align with the magnetic axis. The radiation
beams will sweep around and create the light house
effect. What we observe on Earth will be pulses of
radio wave with very stable period. This is a pulsar.