Classification of stars Flashcards

Revision (35 cards)

1
Q

how many arc seconds in an arc hour

A

its called a degree not an arc hour and 3600

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2
Q

Name 3 methods of determining distance to stars

A

1: Stellar parallax, 100-1000pc
standard candles
2: type 1a super nova
3: Cepheid Variables, 1kpc to 50 Mpc

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3
Q

define apparent and absolute magnitude

A

Apparent: The apparent magnitude (m) of a star is
the brightness when viewed from Earth
Absolute: The absolute magnitude (M) of a star is the
apparent magnitude it would have if measured
at a distance of 10 pc from the observer

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4
Q

Define black-body radiation

A

A body that absorbs all wavelengths of
electromagnetic radiation and can emit all
wavelengths of electromagnetic radiation.

(also known as a perfect thermal source)

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5
Q

Luminosity

A

the total energy given out per secon, so its power

depends on radius and surface temperature

(The total energy per unit time radiated
by a black body is proportional to the
fourth power of its absolute
temperature) 
stefans law:     L=σAT^4
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6
Q

can you describe continuous, emission and absorption spectra

A

good job if you can if not ha ha

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7
Q

emission and absorption spectra occur due to…..

A

excitation and de-excitation of electrons

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8
Q

absorption and emission of visible light is part of the….

A
Balmer series
( to emit balmer lines the electron in a hydrogen atom must be in the n=2 state)
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9
Q

hey neddy ayla

A

Oh Be A Fine Girl Kiss Me

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10
Q

spectral classes

A

O: Blue 25,000 - 50,000 He+, He, H
B: Blue 11,000 - 25,000 He, H
A: Blue-White 7,500 - 11,000 H (strongest) ionised metals
F: White 6,000 - 7,500 Ionised metals
G: Yellow-White 5,000 - 6,000 Ionised & neutral metals
K: Orange 3,500 - 5,000 Neutral metals
M: Red <3,500 Neutral atoms, TiO

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11
Q

can you describe a Hertzsprung-Russell diagram

A

well you better learn how to then

Notice that:-
the temperature scale is decreasing (50,000 K to
2,500 K).
the classes of star are placed alongside the
temperature scale;
the luminosity scale is logarithmic to compress
it;

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12
Q

Red Giants

A

Objects that have a high luminosity and a low
surface temperature must have a large surface
area. (Stefan’s Law)
 These stars are called red
giants and are found in
the top right corner of
the HR diagram.

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13
Q

White Draves

A

Torbjörn’s dad?

Objects that have a low luminosity and a high
surface temperature must have a low surface
area. (Stefan’s Law).
 These stars are called
white dwarfs and lie in
the bottom left hand
corner of the HR
diagram.
 White dwarfs are stars at
the end of their lives,
where all of their fusion
reactions have stopped
and are they are just
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14
Q

stellar evolution in one slide

A
Stars are formed from great
clouds of gas and dust, most of
which is the remnants from
previous supernovae.
 When the clumps get dense enough, the cloud
fragments into regions called protostars that
continue to contract and heat up.
 Eventually the temperature at the centre of the
protostar reaches a few 106K and hydrogen
nuclei start to fuse together to form helium
The fusion of hydrogen
releases enough energy to
create enough radiation
pressure to stop the
gravitational collapse.
 The star has now reached the
main sequence and will
remain there while it fuses
hydrogen to helium
(continued on slide 2)
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15
Q

stellar evolution the second half

A

Stars spend most of their lives
as main sequence stars.
As the star ages more and
more helium builds up in the
core.
Eventually all the hydrogen is
gone and you are left with a
core of only helium
When the hydrogen in its core runs
out, the outward radiation pressure
stops, gravity wins and the core
starts to contract.
 As the core contracts it heats up.
This raises the temperature of
hydrogen surrounding the core
enough for it to fuse.
When the helium runs out, the carbon-oxygen
core contracts again  shell helium “burning”.
For stars with mass similar to the of the Sun, the
carbon-oxygen core isn’t hot enough for fusion.
The core continues to contract until electrons
exert enough pressure to stop it collapsing
further

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16
Q

ejecting your outer layer

A
The helium shell becomes more
and more unstable as the core
collapses.
 This causes the star to pulsate and
eject its outer layers into space
  planetary nebula.
 A hot dense solid core is left
behind
  white dwarf.
17
Q

a short but exiting life

A

is what stars of greater than 8 solar masses get

18
Q

how i want to die sadly im not a star :(

A

The radiation pressure rapidly decreases so gravity wins
and a rapid collapse occurs until the radius of the inner
core reaches about 30 km.
 Further collapse is stopped by strong force interactions
and the degeneracy pressure of neutrons
The in-falling matter, rebounds off the core producing
a shock wave that propagates outward 
SUPERNOVA

19
Q

how fat you are determines how your life will go

relative masses and the corresponding product at the end of the stars life

A

If the mass of the core is < 1.4 MΘ then a white dwarf
is formed.
If the mass of the core is > 1.4 MΘ then a neutron
star is formed.
If the mass of the core is > 3.0 MΘ then a black hole
is formed.
Important: Note that these values are for the mass of
the core left over – not the initial mass of the star.
Note: The 1.4 MΘ limit is known as the
Chandrasekhar limit

20
Q

Describe and name the coolest(not literally) star in the known universe

A

Neutron Stars
The core gets so dense that it overcomes the
electron degeneracy pressure.
Electrons are squashed onto the atomic nuclei
and combine with protons to form neutrons
A density is reached when the repulsive force of
the neutrons is sufficient to stop the collapse of
the stellar core  neutron degeneracy pressure.

can emit radio waves if oriented correctly they can be observed as pulsars because they pulse

21
Q

We are about to go where the sun doesn’t shine

A

Black Holes
There is no known force in nature that can stop
the collapse of cores greater than 3 solar masses.
The collapse continues until the core contracts
to an infinitely dense point known as a
singularity.
Even light cannot escape from the core within a
certain radius called the Schwarzschild Radius.

22
Q

event horrizon

23
Q

The Schwarzschild Radius

A

radius of Vesc

24
Q

how do we know black holes are there

A

matter falling into them

objects orbiting around them

25
calculating the density of a black hole
use The Schwarzschild Radius as its radius
26
Type 1a super nova
The white dwarf reaches a larger mass, approaching the Chandrasekhar limit  But just before it would collapse into a neutron star (within 1% of the limit), the temperature and density inside the core increase enough to allow the fusion of carbon to take place. Within a few seconds, a substantial fraction of the matter in the white dwarf undergoes nuclear fusion, releasing enough energy (1–2 × 1044 J) to produce a supernova explosion.
27
type 1a super nova the standard candle
``` It’s a standard candle, which means all have the same peak absolute magnitude, M  That means the apparent magnitude can be measured.  Therefore, we can determine the distance using distance modulus…... ```
28
why is the luminocity curve of a type 1a super nova predictable
The light curve of a type Ia supernova is predictable as | it is due to the decay of Ni56 and Co56 isotopes
29
O
25000-50000 Blue He+, He, H
30
B
11000-25000 Blue He,H
31
A
7500-11000 Blue-White H(strongest) ionized metals
32
F
6000-7500 White Ionized metals
33
G
5000-6000 Yellow-White Ionized and Neutral metals
34
K
3500-5000 Orange Neutral metals
35
M
2500-3500 Red Neutral atoms, TiO