Exam 2 pt 3 Flashcards

1
Q

summary of pt 2

A

Star formation begins with fragmenting, collapsing cloud of dust
and gas.
Collapsing cloud fragments and protostars have been observed.
When the core is sufficiently hot, fusion begins.
Mass determines where a star falls on the main
sequence.
The cloud fragment collapses due to its own
gravity, and its temperature and luminosity increase.
One cloud typically forms many stars, as a star
cluster.

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2
Q

What is a T-Tauri star?

A

A protostar about to become a star Explanation: T-Tauri stars often show jets of gas emitted in two directions — “bipolar
flow” — suggesting they are not yet stable.

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3
Q

Stages of Star Formation

A

Notice how the temperature increases as the diameter
decreases.
Stages 2&3 are relatively quick compared to other stages

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4
Q

Leaving the Main Sequence

A

Once a star has reached the mainsequence stage of its life, it derives its
energy almost entirely from the
conversion of hydrogen to helium via the
process of nuclear fusion in its core.
H~90% of star’s composition, so all stars
remain on the main sequence for most of
their lives.
Fusion does not change the total mass of the star appreciably, but it does change
the chemical composition in its central regions: hydrogen is gradually depleted,
and helium accumulates.

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5
Q

Main Sequence Equilibrium

A

Dynamic interplay between outward pressure and inward gravity. If the fusion core of the
star heats up the
outward pressure
causes expansion. The star cools when it
expands, thus controlling
the temperature and
restoring the balance.

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6
Q

Stellar Fuel Consumption

A

While on the main sequence, the composition of a star’s core is changing. Fusion converts H to
He mainly in the core.
The inner core of non-burning
He grows significantly.
When the hydrogen supply dwindles, the fusion reaction can no longer supply a counterbalancing
force to that of gravity. Structural changes begin and the star evolves off of the main sequence
(about 10 billion years after the star arrived on the main sequence).

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7
Q

Evolution of our Sun

A

Later evolutionary stages bring changes to our Sun’s size and color.
Central temperature starts to increase from internal changes to the star.
Radius of star also changes!
Ultimate fate of the star depends on its mass.

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8
Q

Stage 8

A

Subgiant status - 100 million years
As the fuel in the core depletes, the core contracts;
when it is used up the core begins to collapse.
Hydrogen begins to fuse in a shell outside the core.
Energy production actually increases and the star
gets brighter.
Increased outward pressure expands the nonburning gaseous exterior of the star.
The layers expand and cool. R~3R⦿.

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9
Q

Stage 9

A

Red Giant Status
Despite its cooler temperature, its luminosity
increases enormously due to its large size.
It is now a red giant, extending out as far as the
orbit of Mercury.
R~100R⦿. L~2,300L⦿.
The He core is tiny - several Earths in diameter, but
it contains 25% of the stellar mass.
The star cools, so it moves to the right on the H-R
diagram. It gets brighter so it moves upward as well

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10
Q

Stage 10

A

The helium flash:
Helium begins to fuse extremely rapidly; within hours
the enormous energy output is over, and the star once
again reaches equilibrium.
Once the core temperature has risen to
100,000,000 K, the helium in the core starts to
fuse into carbon.
Surface temperature is up slightly compared to stage
8/9. Star ends up on the horizontal branch. R~10R⦿.
Core expansion and cooling from the He-flash
ultimately reduces luminosityn.

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11
Q

Stage 11

A

Back to the Giant Branch - asymptotically. As the helium in the core fuses to
carbon and oxygen, the core becomes
smaller and hotter, and the helium burns
faster and faster. The star is now similar to its condition just
as it left the main sequence, except now
there are two shells. Incredible outward pressure swells the
gaseous part of the star. R~500R⦿.

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12
Q

Stage 11 - HR Diagram

A

The star has become a red giant for the second time. The fusion shells make the star expand again, it
increases in luminosity and cools slightly. Thus it
moves up and to the right on the H-R diagram
again. The He-Carbon core shrinks.
Because of its small size (1M⦿), the core
temperatures do not go above 600 million K
needed to start carbon fusion. (This is a Sun-like star, but heavier stars continue
with more fusion shells…stay tuned…)

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13
Q

Summary

A

Evolution of a 1M⦿ star
* Once hydrogen is gone in the core, a star burns
hydrogen in the surrounding shell.The core contracts
and heats; the outer atmosphere expands and cools.
* Helium begins to fuse in the core, as a helium flash.
The star expands into a red giant as the core
continues to collapse.

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14
Q

During formation, the Sun evolved toward the main sequence as shown in the
figure. The Sun will evolve away from the main sequence when

A

Helium builds up in the core, while the hydrogen-burning
shell expands.

Explanation: When the Sun’s core becomes unstable and contracts, additional H
fusion generates extra pressure, and the star will swell into a red giant.

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15
Q

Star Clusters

A

We observe star clusters to test our models of stellar evolution since no star evolves to a red giant quickly enough to watch directly.

Globular clusters: These are nearly round and contain hundreds of thousands of mostly orange and red stars.
Open clusters: These have irregular shapes and contain a few dozen to several hundred stars, with a range of ages among them.

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16
Q

Evolution of Star Clusters

A

A series of H–R diagrams shows how stars of different masses, but the same age, change as the cluster ages. After 10 million years, the most massive stars have already left the main sequence, while many of the least massive stars haven’t even reached it. Astronomers use the top of the main sequence, called the turnoff point, to estimate a cluster’s age.

17
Q

Evolution of Star Clusters

A

After 100 million years, a clear main-sequence turnoff appears, showing the highest-mass stars still on the main sequence. By 1 billion years, this turnoff is even more distinct. After 10 billion years, several new features are visible: the subgiant, red giant, horizontal, and asymptotic giant branches are all well-populated.

18
Q

Evolution of Massive Stars

A

Stars more massive than the Sun follow very different paths when leaving the
main sequence. High-mass stars, like all stars, leave the main sequence
when there is no more hydrogen fuel in their cores. Luminosity does not change much as they swell and
shrink. Only the temperature changes. 4M⦿ and 10M⦿ do NOT undergo He flashes.
Get red and blue supergiants

19
Q

Red Supergiants

A

Element Fusion-The first few events are similar to those in
lower-mass stars – first a hydrogen shell, then
a core burning helium to carbon, surrounded
by helium- and hydrogen-burning shells.
Element Fusion
10M⦿ get hot enough to fuse He+C into
Oxygen
Heavier stars can fuse elements up to iron.
Betelgeuse in Orion is a red super giant.
L=10,000L⦿.

20
Q

High Mass Star Life Cycle

A

In heavy mass stars, He fusion starts quickly - before the star can become a
red giant
Subsequent fusion reactions happen faster and faster.
A 20M⦿ star burns:
H for 10 million years
He for 1 million years
C for 1000 years
O for 1 year
Si for a week
Iron core grows for less than a day!
S
Once the iron core builds up, the stellar fusion ceases.
Gravity overwhelms the pressure of the hot gas and the star collapses.
Core temperature rises to 10 billion K!

21
Q

Star Deaths-Stage 13 - White Dwarf Status

A

Fusion ceases, the envelope blows off, leaving a white dwarf to slowly cool. White dwarf - new force stops the
core collapse from the pull of gravity
Electron pressure - Since electrons are identical
particles, the Pauli Exclusion Principle states that they
can not occupy the same space.
Thus the electron “wave functions” push each other
away and create an outward pressure The Hubble Space Telescope has detected white dwarfs in globular clusters

22
Q

Stage 14 - Black Dwarf

A

White dwarf continues to cool.
No more contraction due to electron pressure.
Remains the size of Earth.
Temperature approaches zero K!
After a trillion years or so, the dead star
becomes a cold, dense, burned-out cinder in space.
Since the age of the universe is about 14 billion
years old, no black dwarfs are expected to exist yet

23
Q

Stars like our Sun will end their lives as

A

White dwarfs

24
Q

Massive stars’ death

A

Only stars with a end life mass of less than 1.4 times the mass of the Sun (called
Chandrasekhar limit) will end their cycle as white dwarfs.At the latest stage of its evolution, a massive
star resembles an onion with an iron core. As
we get farther from the center, we find shells
of decreasing temperature in which nuclear
reactions involve nuclei of progressively
lower mass: silicon and sulfur, oxygen, neon,
carbon, helium, and finally, hydrogen.

25
Q

Neutron star

A

When the density reaches 4 × 10^11g/cm,some electrons are actually squeezed
into the atomic nuclei, where they combine with protons to form
neutrons and neutrinos. The collapsing core can reach a stable state as
a crushed ball made mainly of neutrons, which
astronomers call a neutron star. We don’t
have an exact number (a “Chandrasekhar
limit”) for the maximum mass of a neutron
star, but calculations tell us that the upper
mass limit of a body made of neutrons might
only be about 3MSun

26
Q

Supernovae

A

A supernova is a one-time violent explosion – once it happens, there is little
or nothing left of the progenitor star.There are two types of Supernova Explosions
Supernova are spectroscopically
defined
Type II, which is the core-collapse
death of a high-mass star (M > 12 M⦿)
and have H lines in spectra
Type Ia, posses Si lines in the spectra
Type Ib, posses He lines in the
spectra
Type Ic, anything else
Remember novae are NOT supernovae.
Supernovae (1010 solar units) are more than a million times as bright
as a novae (104 solar units).

27
Q

Type II Supernova

A

Fusion of iron ceases. Core temperature is ~ 10 billion K!
The core photo-disintegrates in less than a second into its constituents.
Core collapses until the neutrons “bump into
each other” and create a rebounding pressure.
(1015-1018 kg/m3)! This is a shock wave.
Total amount of energy radiated in blast equal to the Sun’s output over its entire life!
Protons and electrons are crushed together
creating neutrons and neutrinos: core becomes a
neutron star.

28
Q

Supernova Remnants

A

Send the star’s remnants back into space.
Shell of hot gas radiates in the x-ray
spectrum.
Analysis of the x-rays reveal dynamics
of the explosion and the elements
produced by the star.

29
Q

black hole and type II supernovae

A

If a core remnant is more massive
than 3M Sun, nothing will stop its
collapse, and it will become smaller
and smaller and denser and denser.
Eventually the gravitational force is
so intense that even light cannot
escape. The remnant has become a
black hole

30
Q

Type Ia Supernova

A

Carbon-detonation supernova:White dwarf that has accumulated too much
mass from binary companion. (A recurrent nova can go supernova this way.) If the white dwarf’s mass exceeds 1.4 solar masses (Chandrasekhar mass), electron
degeneracy can no longer keep the core from collapsing.
Carbon fusion begins throughout the star almost simultaneously, resulting in a carbon
explosion.

31
Q

Type I Supernova

A

Type Ia Supernovae are standard candles, used as a distance measure
Type Ia are standard candles:
objects of known brightness
Given a standard candle, we can
measure the apparent brightness,
and use the inverse square law to
determine the distance of these
objects

32
Q

Novae

A

Star that flares up very suddenly and then returns slowly to its former
luminosity.
* Must be part of a binary system.
* See two or three per year.
* Turns on over the period of days.
* Lasts for months
A white dwarf that is part of a semi-detached binary system can undergo
repeated novas.
When enough material has accreted, surface
fusion can reignite very suddenly, burning off the
new material quickly and violently.
Material keeps being transferred to the white
dwarf, and the process repeats.
Material falls onto the white dwarf
from its main-sequence companion.

33
Q

Novae Evidence

A

Nova Persei
a) 50 years after after being brightened
by a factor of 40,000 in 1901
b) Nova Cygni (HST image)
erupted in 1992
left - 1 year after blast
right - 7 more months later

34
Q

A white dwarf can explode when

A

Its mass exceeds the Chandrasekhar limit. Explanation: If additional mass from a companion star pushes
a white dwarf beyond 1.4 solar masses, it can explode in a Type I supernova

35
Q

Stellar Evolution Cycle

A

Star formation is cyclical - stars form, evolve, and die. In dying, stars send heavy elements
into the interstellar medium.
These elements then become parts
of new stars.
And so it goes.