Chapter 7 Flashcards

1
Q

What is the structure of a sub-giant branch star?

A

H burning takes place in core and gets exhausted from inside out, leaving a H burning shell around the core

He rich core grows outwards and becomes larger and contracts to regain hydrostatic equilibrium (pressure goes up in core)

Expanding photosphere

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2
Q

What is the temperature of the core of the sub-giant branch?

A

2 x 10^7 K which is sufficient for surrounding H to burn via CNO cycle

T^16 dependence which lead to thin H burning shell

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3
Q

Why is the core of a star entering the sub-giant branch so hot?

A

In order to maintain pressure balance but this causes H-rich envelope to expand with L being constant and R increasing while T decreases

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4
Q

Where does the star move in the HR diagram to reach the sub-giant branch?

A

redwards

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5
Q

What are the central temperatures of sub giants still too low for?

A

Helium burning to occur in centre at this stage

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6
Q

When does the star move upwards in HR diagram to Red Giant Branch?

A

As surface layers cool due to expansion of envelope, the convection zone deepens into the star
Convection is more efficient at transporting the energy than radiation so L increases and T is now constant

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7
Q

What confirms the CNO cycle in red giant branch?

A

Enhanced 14N/12C and 13C/12C ratios observed in spectra of red giants

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8
Q

What kind of envelope does a red giant have?

A

An extensive fully convective envelope

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9
Q

When can the ideal gas law (P= rRT/μ) break down?

A

When pressure and density continue to increase in contracting He core and at a given temp

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10
Q

What do free electrons do as density increases?

A

The free electrons try to fill all available quantum states

Electrons are fermions with spin=1/2

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11
Q

What is Pauli’s exclusion principle?

A

A given quantum cell can have at most 2 electrons (oppositely directed spins)

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12
Q

What does not obey Pauli’s exclusion principle?

A

Helium nuclei as they have spin 0

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13
Q

What does the restriction on electrons from Pauli’s principle lead to?

A

A pressure greater than that for an ideal gas

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14
Q

What kind of electrons can co-exist in an orbital?

A

Only electrons of opposite spin

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15
Q

From Heisenberg’s uncertainty principle how many electrons are predicted to be able to occupy an “uncertainty” volume of 6-dimensional phase space?

A

At most 2 electrons which gives a volume of a quantum cell equal to h^3

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16
Q

What is volume occupied by particles with momentum equal to in spherical coordinates?

A

4pip^2dp

in 6D phase space: Vxyz x 4pip^2dp

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17
Q

When does the Maxwellian distribution violate the Pauli exclusion principle?

A

For a sufficiently high particle density at low momenta

first do so at p=0 when n (number density of electrons) is at its maximum

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18
Q

What happens as the core contracts?

A

Density increases for given T and the low momentum electrons hit the degeneracy limit first

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19
Q

What happens as degeneracy limit cannot be exceeded?

A

The electrons need to re-distribute to high momentum i.e higher pressure

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20
Q

When does degeneracy increase until?

A

Only the high momentum tail of the Maxwellian distribution is left

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21
Q

What happens to the quantum states are degeneracy increases?

A

All available quantum states will fill up to some maximum momentum p0 (Fermi momentum)

22
Q

When is gas called completely degenerate?

A

When there are negligible number of electrons with p>p0

23
Q

How can degeneracy be removed?

A

By increasing the temperature and hence average momentum of the electrons

24
Q

What is the Fermi momentum?

A

The maximum momentum in a degenerate gas which depends on the density

25
Q

What is pressure due to?

A

Degenerate electrons

Pressure is independent of temperature

26
Q

What happens at the tip of RGB?

A

He core is completely degenerate and T reached 10^8K which leads to triple a reactions to start

27
Q

What causes the runaway process, helium flash?

A

The pressure does not increase initially as RGB He core become completely degenerate, because pressure is only a function of density and not of temperature

28
Q

What do runaway reactions cause?

A

The temperature to increase and it populates the Maxwellian electron distribution, starting with the high energy tail.

Degeneracy is lifted and pressure increases

29
Q

What causes star to move from RGB to Horizontal branch after runaway reactions?

A

Core expands leads to envelope contraction so R decreases and T increases

Density and T in shell decrease so L decreases

30
Q

In order to maintain pressure balance what happens to the envelope which is contracting?

A

The density of it goes up

31
Q

What does the initial position on HB of Horizontal branch depend on?

A

Metallicity

RED END: metal rich (young Pop I)
BLUE END: metal poor (old Pop II)

32
Q

What is the structure of a horizontal branch star?

A

He burning in core which CO in centre builds up
He intershell
H burning shell
envelope

33
Q

How does star ascend from HB to Asymptotic Giant Branch (AGB)?

A

As the core contracts and envelope expands, T decreases and convection zone deepens
Efficient convection means L increases

34
Q

What is the structure of AGB star?

A

CO core
He burning shell
H burning shell
H and He envelope

35
Q

What usually dominates Ls on AGB?

A

H burning shell

This causes a thermal pulse (occurs with increasing frequency)

36
Q

When do runaway reactions occur again(He flash)?

A

When there is a build up of pressure in he burning shell

37
Q

What happens after He flash?

A

Envelope expands and cools, giving rise to less H burning, which increases when core is shrinking again
This slowly increases again as He flash dumped on core

38
Q

What happens after thermal pulses?

A

Surface is now cool enough (T = 3000K) and dense enough for dust to form in atmosphere

39
Q

What gives rise to dense stellar wind?

A

Combination of pulsation and radiation pressure on dust

40
Q

How long does it take dense wind to eject envelope?

A

around 10^4 yrs

41
Q

When does Teff rise rapidly?

A

When remnant H or He burning shell now very close to surface
Core continues to contract

42
Q

When is a planetary nebula formed?

A

When Teff > 30,000K and the stellar remnant can ionize ejected envelope

43
Q

What is the structure of the planetary nebula?

A

Nebula has an emission line spectrum

Abundances in nebula reflect CNO processed (enhanced He and N) and triple a process (enhanced C) material

44
Q

What eventually happens to planetary nebula?

A

It expands and eventually disperses into the interstellar medium

(very few old PNe have been observed as they are so faint)

45
Q

How long does it take a planetary nebula central star to run out of H or He in remnant shell?

A

Around 10^4-5 years

46
Q

What happens after planetary nebula runs out of H and He?

A

Core contracts again
Central T and density never get high enough for C burning
Degenerate CO core then cools and L decreases
Surface is left either H or He rich

47
Q

What is the expansion speed of the PN material?

A

Around 20-30km/s which should be at least as large as the escape speed

48
Q

What is strange about the observed expanding material?

A

It’s speed is around 20 km/s so it couldn’t have been ejected from PN central star.
So PN material was probably ejected during an earlier phase

49
Q

When do white dwarfs reach a maximum mass?

A
When all (degenerate) electrons are pushed to relativistic velocities 
Mass = 1.4Mo (known as Chandrasekhar mass)
50
Q

Which type of stars go through the AGB and PN stages?

A

Low to intermediate mass stars (0.8 to 8 Mo)

51
Q

What do stars that go through the AGB and PN stages return?

A

A large fraction of their mass to the interstellar medium enriched in heavy elements

52
Q

What is the stellar remnant?

A

A CO white dwarf