Download Unit 1

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

International Ultraviolet Explorer wikipedia , lookup

History of Solar System formation and evolution hypotheses wikipedia , lookup

Canis Minor wikipedia , lookup

Formation and evolution of the Solar System wikipedia , lookup

Auriga (constellation) wikipedia , lookup

Star of Bethlehem wikipedia , lookup

Observational astronomy wikipedia , lookup

Corona Australis wikipedia , lookup

Boötes wikipedia , lookup

Corona Borealis wikipedia , lookup

Serpens wikipedia , lookup

Nebular hypothesis wikipedia , lookup

Cassiopeia (constellation) wikipedia , lookup

Dyson sphere wikipedia , lookup

Ursa Major wikipedia , lookup

Star catalogue wikipedia , lookup

Planetary habitability wikipedia , lookup

Cygnus (constellation) wikipedia , lookup

Hipparcos wikipedia , lookup

Aquarius (constellation) wikipedia , lookup

Perseus (constellation) wikipedia , lookup

P-nuclei wikipedia , lookup

Stellar classification wikipedia , lookup

CoRoT wikipedia , lookup

Future of an expanding universe wikipedia , lookup

Astronomical spectroscopy wikipedia , lookup

Star wikipedia , lookup

Lyra wikipedia , lookup

Timeline of astronomy wikipedia , lookup

H II region wikipedia , lookup

Stellar kinematics wikipedia , lookup

Hayashi track wikipedia , lookup

Corvus (constellation) wikipedia , lookup

Ursa Minor wikipedia , lookup

Star formation wikipedia , lookup

Stellar evolution wikipedia , lookup

Transcript
Units to cover: 62, 63, 64
Homework:
Unit 60: Problems 12, 16, 18, 19
Unit 61 Problems 11, 12, 17, 18, 20
Unit 62 Problems 17, 18, 19
Unit 63, Problems 17, 19
Internal Structure of Stars - Convection
• Convection occurs in the
interiors of stars
whenever energy
transport away from the
core becomes too slow
– Radiation carries away
energy in regions where
the photons are not
readily absorbed by
stellar gas
– Close to the cores of
massive stars, there is
enough material to
impede the flow of
energy through radiation
– In less massive stars like the Sun, cooler upper
layers of the Sun’s interior absorb radiation, so
convection kicks in
– The lowest-mass stars are fully convective, and
are well mixed in the interior.
The Main-Sequence Lifetime of a Star
• The length of time a star spends fusing
hydrogen into helium is called its main
sequence lifetime
– Stars spend most of their lives on the main
sequence
– Lifetime depends on the star’s mass and luminosity
• More luminous stars burn their energy more rapidly
than less luminous stars.
• High-mass stars are more luminous than low-mass
stars
• High mass stars are therefore shorter-lived!
• Cooler, smaller red stars have been around for a
long time
• Hot, blue stars are relatively young.
Two Young Star Clusters
How do we know these clusters are young?
Stellar Evolution on the Main Sequence
A Reminder of a Star’s Internal Processes
• The balance of forces in
the interior of a star is
delicate, though stable for
millions or billions of
years.
– A star acts like it has a
thermostat
– If internal temperature
decreases, internal
pressure decreases, and
the star collapses a little,
raising the temperature
• When hydrogen in the
core is exhausted, the
thermostat breaks…
Evolution to red giant phase
• The star is expanding and cooling, so its
luminosity increases while its temperature
decreases
• Position on the HR diagram shifts up and
to the right…
Evolutionary tracks of giant stars
CNO cycle happens
A. In protostars as they are not hot enough
B. In the stars similar to our Sun
C. In high mass stars with very hot core
D. In fully convective low mass stars
When a star leaves the main sequence and expands
towards the red giant region, what is happening
inside the star?
• a. Hydrogen burning is taking place in a spherical
shell just outside the core; the core itself is almost
pure helium.
• b. Helium is being converted into carbon and oxygen
in the core.
• c. Helium burning is taking place in a spherical shell
just outside the core.
• d. hydrogen burning is taking place in a spherical
shell, while the core has not yet started thermonuclear
reactions and still mostly hydrogen.
Helium Fusion
• Normally, the core of a star is not hot
enough to fuse helium
– Electrostatic repulsion of the two
charged nuclei keeps them apart
• The core of a red giant star is very
dense, and can get to very high
temperatures
– If the temperature is high enough,
helium fuses into Beryllium, and then
fuses with another helium nuclei to
form carbon.
A (temporary) new lease on life
• The triple-alpha
process provides a
new energy source
for giant stars
• Their temperatures
increase
temporarily, until
the helium runs out
• The stars cool, and
expand once again
• The end is near…
Light Curves
• To characterize the
variability of a star,
scientists measure the
brightness, and plot it as a
function of time.
– Light Curves
• Different kinds of
variability
– Irregular Variable
• Novae (death)
• T Tauri stars (birth)
– Pulsating Variable
• Periodic changes in
brightness
Yellow Giants and Pulsating Stars
• If you plot the positions of variable stars on the HR diagram,
many of them fall in the “instability strip”
– Most have surface temperatures of ~5000K, so appear yellow
– Most are giants (Yellow Giants)
– Instability comes from partial absorption of radiation in the interior
of the star
• Helium absorbs radiation, and the outer layers of the star get pushed away
from core
• As the star expands, the density decreases, letting photons escape
• Outer layers head back inward toward core
• Repeat
– RR Lyrae and Cepheid variables are useful for finding distances to
the stars, as the star’s period is proportional to its luminosity.
The Valve Mechanism
A Cepheid variable is
• a. a low mass red giant that varies in size and
brightness in an irregular way
• b. a big planet
• c. a high-mass giant or supergiant star that pulsates
regularly in size and brightness
• d. a variable emission nebula near a young star
The Life-path of the Sun
Formation of Planetary Nebula
• As a red giant expands, it cools
– Outer layers cool enough for carbon
flakes to form
– Flakes are pushed outward by
radiation pressure
– Flakes drag stellar gas outward with
them
– This drag creates a highspeed stellar wind!
– Flakes and gas form a
planetary nebula
The Hourglass Nebula
White Dwarf Stars
• At the center of the
planetary nebula lies the
core of the star, a white
dwarf
– Degenerate material
– Incredibly dense
• Initially the surface
temperature is around
25,000 K
• Cools slowly, until it
fades from sight.
Figure 64.05e
Our Sun will end its life by becoming
•
•
•
•
A. a molecular cloud
B. a pulsar
C. a white dwarf
D. a black hole
Mass Transfer and Novae
• A Roche lobe can be
seen as a sphere of
gravitational
influence around a
star
• Red Giant stars can
fill their Roche lobes
• In a binary star
system, the Roche
lobes of the two stars
can touch, and mass
can pass between
them.
• If a white dwarf is in orbit around a red giant
companion star, it can pull material off the
companion and into an accretion disk around itself
• Material in the accretion disk eventually falls to the
surface of the white dwarf
Novae
• If enough material accumulates on the white dwarf’s
surface, fusion can be triggered, causing a massive
explosion
• This explosion is called a nova
• If this process happens repeatedly, we have a recurrent
nova.