galaxies Flashcards

1
Q

What is a galaxy?

A

An enormous collection of stars held

together by their common gravity.

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2
Q

some details on galaxies

A

 Galaxies have a wide range of masses: from 100 m stars (dwarf galaxies) to >1 t stars (giant galaxies).  Lower mass galaxies are more common.  Galaxies have a wide range of ages, stellar populations (the mix of stars in a galaxy), and gas content.

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3
Q

Anatomy of the Milky Way

A

The Milky Way (like any spiral galaxy) consists of:
 A central bulge
 A disk: extremely wide, but very thin
 Disk diameter: 100,000 l.y. = 100 kl.y. (30 kpc )
 Disk thickness: 1,000 l.y. = 1 kl.y. (300 pc)  A large halo which surrounds almost completely the entire disk

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4
Q

how many stars in milky way

A

~100 b stars (up to 1 t )

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5
Q

where is milky located in the galaxy

A

 Our solar system is located in the disk, 28,000 light years (=28 kl.y.) from centre  Being situated in the plane of the disk we cannot observe clearly the structure of the Milky Way. Moreover, dusty gas clouds obscure our view because they absorb visible light. This is the interstellar medium that makes new star systems.

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6
Q

arms

A

Previously, our galaxy was thought to have 4 major arms.

In 2008, it was announced that IR images from NASA’s Spitzer Space Telescope have shown that the Milky Way’s elegant spiral structure is dominated by just 2 major arms wrapping off the ends of a central bar.  It is orbited by a few small and very small galaxies (among them the Magellanic clouds are the most representative)

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7
Q

Contents of the Milky Way

A

disk
bulge
halo

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8
Q

Disk:

A

Filled with interstellar gas & dust ≡ interstellar medium (ISM), made up of H gas (atomic & molecular) & dust  Younger stars  Open clusters

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9
Q

Bulge:

A

 Filled with denser gas & dust Young & older stars @ high density  A few globular clusters may also be present here

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10
Q

halo

A

 No gas/dust, or very rarified (tenuous) Old stars  Globular clusters

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11
Q

Milky Way = typical . . .

A

all spiral galaxies have the

same structure

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12
Q

small galaxy companions

A

Milky Way’s strong gravity influences smaller galaxies

in its vicinity

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13
Q

small galaxy companions, The most important

A

the Large Magellanic Cloud (LMC), and  the Small Magellanic Cloud (SMC), Both are irregular galaxies and much smaller than the Milky Way

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14
Q

Other small galaxy companions:

A

The Sagittarius Dwarf Elliptical Galaxy (SagDEG) → a small elliptical galaxy Canis Major Dwarf Galaxy: the closest known satellite galaxy but well hidden behind banks of dust in the plane of the Milky Way

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15
Q

Our galaxy’s tidal forces will ultimately

A

rip apart & ‘cannibalize’ these 2 small companions in ~1 b yrs

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16
Q

Stars in disk

A
  • relatively young.

 Plenty of high- & low-mass stars, blue & red  Fraction of heavy elements same as or greater than the Sun

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17
Q

Stars in halo are old

A

formed early in Milky Way’s history
 Mostly low mass, red stars
 Fraction of heavy elements much less than the Sun → Formed when few heavy elements existed
 Star formation stopped long ago when all gas flattened into disk  No (or extremely little) ISM in the halo The fact that the stars in the disk have very different origins than those in the bulge & halo is also reflected in great differences between their galactic orbits .

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18
Q

All stars in the disk orbit around the galactic centre.

A

 Circular motion of all stars in disk orbits → arises from gravitational attraction towards galactic centre
 It is always in the same direction & in the same plane (roughly)
 There is “bobbing” up & down due to the localized disk gravity → defines disk thickness

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19
Q

All stars in bulge &
halo also orbit around
the galactic centre, but…

A

 They have random orientations: different directions (even opposite!) at various inclinations to disk  Higher velocities & orbits are elliptical, sometimes at great distances from center

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20
Q

Orbital motions of mass in spiral arms of galaxies indicate that most of their mass is

A

NOT concentrated near the galactic centre, but the opposite is true .  If most mass were concentrated in the center, the stars closer to the centre would orbit very fast, those more distant would orbit slower  Measurements indicate that orbital speeds remain constant even up to great distances from the centre

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21
Q

Most of the galaxy’s mass resides far from the center

A

is distributed throughout the halo

There is little gas or dust, very few stars and no emitted light from the halo →  Most of a galaxy’s mass is due to the presence of dark matter
 it has a large mass-to-luminosity (M/L) ratio

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22
Q

Galactic recycling is essential for the formation of stars

.

A

 Recycles material from old stars into new ones: the birth of the Sun & the Solar System could not have occurred without it.  Takes place within the disk of the galaxy & its ISM

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23
Q

Galactic recycling gradually changes the chemical composition of
the ISM.

A

 With each cycle more heavy elements are made by fusion in stars
 This is the process due to which all heavier elements than H & He have been produced → after 10 b years of recycling, the chemical composition of the ISM is: 70%H2 , 28%He & 2% heavier elements.  Different galactic regions change composition at different rates

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24
Q

How does it take place, and how these chemical riches

produced by stars remained in our galaxy?

A

It is a complex and long process, taking place in several stages

hot bubbles
atomic hydrogen clouds
molecular clouds
star formation
stellar burning/heavy-element formation
supernovae and stellar winds
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25
Q

All stars return much of their material into ISM in 2 ways:

A

 Through stellar winds, and  Death events.

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26
Q

Low mass stars return most of their material into ISM via:

A

Gas ejection through mild stellar winds, and  Mass loss through planetary nebulae

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27
Q

High mass stars return most of their material into ISM via:

A

Massive gas ejection through strong stellar winds,

 Mass loss through supernovae

 Heavy elements forged in (large) stars are thus returned in the ISM & contribute to formation of new stars, planets & appearance of Life

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28
Q

Consequently, low mass stars have much

less effect

A

on the ISM than high mass stars which influence & contribute to it much more significantly

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29
Q

Supernovae eject high-speed gas in a shock wave

A

Sweeps up ISM
 Bubble of hot gas ( > 1 m K) excavated
 Gas is strongly compressed, heated, ionized & excited → emits mainly X-rays, but also visible & IR radiation as it expands & cools
 Some e– accelerated to nearly speed of light as they interact with the shock wave  As these fast e– spiral around mgn. field lines threading the supernova remnant (SNR) → they emit radio waves (this radio emission is sometimes called synchrotron radiation )

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30
Q

 Supernovae also generate cosmic rays

A

highly energetic particles, mainly protons (p +) & atomic nuclei -including some heavy ones- and a few e–, travelling at close to the speed of light

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31
Q

 Our solar system is also in a huge

A

supernova bubble created long

time ago!

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32
Q

Bubbles fill

A

20~50% of Milky Way’s disk

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33
Q

Multiple supernovae can create huge bubbles of hot gas

A

which blow out of the galactic disk.
 In many places in our galactic disk elongated superbubbles
are observed

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34
Q

Multiple supernovae can create huge bubbles of

hot gas part 2

A

 The hot gas has very low densities and temperatures as high as a few m K, hence it is hot enough to emit Xrays → can be observed
The hot gas breaks out of the disk  a blowout like a volcanic eruption
 Part of the disk’s own material is also ejected

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35
Q

Hot gas bubbles/gas clouds cool

in the halo

A

 Energy shared with swept-up ISM matter & also radiated from all shocked gas  Also lose angular momentum

Only gravity slows down gradually the bubble’s expansion & eventually reverses the rise of the gas from the blowout → The galactic fountain model
Cooled gas clouds rain back down onto the disk → merge & impact the ISM in a large region of the disk 
These collisions may trigger future star formation .
Heavy elements also returned & merge into disk’s ISM

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36
Q

What happens As ISM cools

A

p + recombine with e–  neutral atomic H formed (neutral because is cool enough)

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37
Q

Atomic H emits at λ = 21 cm

A

 Radio emission line emitted when spin state of e– flips  Used to map atomic H distribution in disk with radio telescopes

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38
Q

Milky Way has 5 b MSun of atomic H.

A

Large, tenuous, 10,000 K warm clouds (1 atom/cm 3)

 Small, dense, 100 K cool clouds (100 atoms/cm 3)

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39
Q

Warm atomic H clouds slowly cool & contract into denser clouds over m of years

A

 Gravity slowly draws gas together into tighter clumps  Energy radiated more efficiently as cloud grows denser

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40
Q

Molecular H 2 forms as atomic H cools from 100 K to 10…30 K.

A

 Molecular clouds created: 70% H2 , 28% He, ~1% CO + many other substances
 No emission from H2 !
 Cold, heavy & dense molecular clouds settle in the central layers of the Milky Way’s disk

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41
Q

Radio emission of other molecules can be observed.

A

H2O, CO (3 mm emission line), NH3 , -OH, alcohol

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42
Q

Supernova explosions disturb the cold molecular clouds

A

stir them up & create turbulences

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43
Q

Gravitational push triggers

A

cloud core formation & their collapse

forms new stars, thereby completing the star-gas-star cycle.

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44
Q

Once a few stars form in a newborn cluster, they begin to hamper the creation of new stars

A

 The molecular cloud is eroded & pushed away by stellar winds & radiation pressure  It is also heated/excited & ionized by UV photons from high-mass stars

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45
Q

Supernovae are crucial for both star & planet formation.

A

 Tremendous amounts of matter blasted into intergalactic space
 Heavy elements created → the production and dispersal of even a small amount could have had a major effect on star & planets formation

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46
Q

Enable creation of stars from protostellar disks.

A

 When the abundance of ‘metals’ in star-forming clouds rises above one thousandth of the metal abundance in the Sun, the metals rapidly cool the gas to the temperature of the cosmic background radiation
  ‘Metals’ are much more effective than hydrogen in cooling starforming clouds → faster & easier collapse into stars

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47
Q

Next generation stars begin life with more heavy
elements
→ numerous advantages:

A

 Nuclear fusion in the star core is less efficient without ‘metals’  otherwise it would have to be hotter and more compact to produce enough energy to counteract gravity
  Because of the more compact structure, the surface layers of the star would also be much hotter: Tsurf ~100,000 K (17× higher than the Sun’s surface temperature)
The heavy elements also enable the creation of planets & appearance of life

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48
Q

Star-gas-star cycle cannot go on forever.

A

 Stellar formation & evolution -> matter gradually “locked” in red dwarfs, brown dwarfs & stellar corpses
 Other material → irretrievably spread out as ISM or intergalactic gas
 Star formation rate will taper off over next 50 b years Eventually, star formation will cease!

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49
Q

Galactic recycling in

the Milky Way

A

The star-gas-star cycle is observed in the Milky Way using many different wavelengths of light

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50
Q

Galactic recycling: SUMMARY

A

Stars make new heavy elements by fusion.
Dying stars expel gas and new elements , producing hot bubbles of gas (~1m K) which emit X-rays .
This hot gas cools, allowing atomic H clouds to form (~100,000-10,000 K).
 Has a 21 cm wavelength emission line. Further cooling  molecules (CO, etc.) form, making molecular clouds (~30 K).
 Observed using CO emission line at 3 mm.
Gravity forms new stars (and planets) in molecular clouds.
 The process starts over again!

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51
Q

Where will our Galaxy’s gas be in 1 trillion years from

now?

A

A. Scattered in ISM and intergalactic space
B. Locked into white dwarfs and low mass stars
C. Both of the above
D. Blown out of galaxy
E. Still recycling just like now

Galactic recycling is an imperfect process. More and more gas gets locked up into low-mass stars and white dwarfs, which never return their material to the ISM, and some material will remain scattered in space and will never have the possibility to collapse & form stars again

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52
Q

Where do stars form in our galaxy?

A

In any galaxy, stars -and also regions of new star formation- are not spread evenly (more dense in gas&dust clouds-rich areas)  Much of the star formation in the galactic disk happens in the spiral arms.

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53
Q

Spiral arms are enormous & prolific & star formation waves propagating through the gaseous disk

A

Stars & clouds more densely packed → Gas clouds get squeezed as they move into spiral arms
 Squeezing of clouds triggers star formation.
 Young stars flow out of spiral arms.
 Supernovae of massive stars compress further the clouds, triggering more star formation.

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54
Q

The disk does not appear solid.

A

Has spiral arms  The arms are not fixed strings of stars

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55
Q

Spiral arms are high density waves propagating through the gaseous disk

A

 Stars & clouds more densely packed
  Prolific star formation activity
 Massive stars, formed as gas clouds pass through spiral arms, die out quickly before completing one galactic orbit → spiral arms appear bluer than the bulge or gaps between arms
 Long-lived yellow & red stars survive many galactic orbits & pass through many spiral arms → more evenly distributed throughout the galactic disk

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56
Q

Halo:

A

 Star formation started first in halo, then stopped
 NO ionization nebulae, NO blue stars
 NO star formation (and hence NO recycling ) →
 Only old stars, and with fewer heavy elements (0.02…0.2%)

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57
Q

Galactic disk

A

 Ionization nebulae, blue stars
 Star formation active →
 Stars of many different ages with ~2% heavy elements
 Disk stars formed later & keep forming!
 Milky Way’s star formation rate is about 1 MSun/yr.
Conclusion: The halo lacked the gas for new star formation for a very long time because it has settled into the disk

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58
Q

The initial most basic model for Milky Way’s formation

(Monolithic Collapse Model):

A

 It was first thought that the galaxy began as a giant protogalactic cloud containing all the H & He gas that eventually turned into stars or is now present in the ISM.
 The protogalactic cloud collapsed and halo stars began to form
 Conservation of angular momentum ensured that the remaining gas flattened into a spinning disk.  Spiral arms then formed and the star-gas-star cycle started supporting ongoing star formation in the disk.

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59
Q

Multiple merger model: Recent data show that our galaxy formed from a few different gas clouds, not just one.

A

 The earliest stars formed in relatively small clouds, each with a few globular clusters.
 These clouds later collided (  rapid star formation in what is now the halo) & created a combined full protogalactic cloud that became the Milky Way.
 Once the protogalactic cloud was in place, it collapsed into the disk and the formation of stars & heavy element enrichment proceeded in a more orderly fashion

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60
Q

The evidence for the multiple merger model

A

the heavy element content of stars in the intermediate layer between the disk & halo depends on their distance from the galactic center

These stars are almost as old as halo stars but formed just before the spinning protogalactic cloud finished flattening into a disk → it had only 10% of the present heavy element content

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61
Q

Old stars in the bulge have a

A

composition similar to that of the Sun, even though their ages exceed 10 b years

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62
Q

The centre of Milky Way lies in the direction of Sagittarius

.

A

 Bulge obscured by ISM  IR & radio views reveals swirling gas clouds & a cluster of several million stars

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63
Q

Bright radio source (with vast threads of emission tracing mgn. field lines) in the centre with occasional Xray flares  Sgr A*.

A

 Hundreds of stars crowded within 1 light-year of the region

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64
Q

Mass in Sgr A*

A

Determined from orbits of fast-moving stars near galactic centre.
 Kepler’s Law gives a mass of ~3.7 m Msun
 This mass is packed into a space a little larger than our solar system

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65
Q

What is so small, yet so massive?

A

A supermassive black hole

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66
Q

The black hole at the centre of our

galaxy has an unusually faint X-ray emission

A

most probably lacks an accretion disk (already gobbled up all material around it)

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67
Q

Life cycles of galaxies are studied the same way as

those of stars:

A

 Impossible to observe continuously from start to end 
Observe galaxies at various stages of their lives
 Life cycles of galaxies are more difficult to study

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68
Q

Studying the lives & evolution of galaxies is impossible without considering the evolution of the Universe

A

The study of galaxies is intimately connected with cosmology = the study of the overall structure & evolution of the Universe

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69
Q

Hubble Space Telescope’s long-distance (far field & ultra far field) observations even in regions apparently

A

utterly empty, devoid of any planets or stars revealed amazing & humbling images of thousands of galaxies.
 The images: the farthest we’ve ever seen into the Universe
 Over 100 b galaxies estimated in the entire Universe! What did the Deep Field observations tell us?
There is a wealth of distant galaxies to be studied!

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70
Q

moon

A

1 s

71
Q

Sun

A

8 minutes

72
Q

Pluto

A

8 hours

73
Q

Nearest star (α Centauri)

A

4 years

74
Q

Sirius

A

8 years

75
Q

Nearest large galaxy (Andromeda)

A

2.5 m years

76
Q

Nearest cluster of galaxies

A

50m years

77
Q

Most distant known galaxy

A

13.4 b years (formed when Universe was 3% of its age, only 407 m y. old. Taking into account the expansion of the Universe, it is now 32.1 b l.y away!)

78
Q

Galaxies classified into 3 types:

A

spiral, elliptical, irregular

79
Q

Spiral

A

 Flat white disk, yellowish bulge

 Cool gas & dust, hot ionized gas

80
Q

Elliptical

A

 Redder, more rounded
 Very little cool gas or dust
 May have very hot ionized gas

81
Q

Irregular:

A

Neither disk-like nor rounded

82
Q

Dwarf galaxies

A

100 m stars

83
Q

Giant Galaxies

A

1 t stars

84
Q

Spiral galaxies  Two primary components:

A

Disk = a thin flat disk (extending outward from the central region, the bulge ) in which stars follow orderly, nearly circular orbits around the galactic centre
 Stars of all ages (including many young ones) & masses
 Appears white, as it contains stars of all spectral types
 Filled with interstellar medium (ISM), made up of H gas (atomic & molecular) & dust
 Active star formation
 Open clusters

85
Q

Spheroidal components

A

(bulge

& halo)

86
Q

Spheroidal components (bulge & halo)

A

the stars within 10 kl.y. of the center belong to the bulge , those outside this radius are members of the halo .

 Stars here have orbits of random orientations: different directions (even opposite!) & shapes (even highly elliptical) at various inclinations

87
Q

Bulge:

A

 Filled with denser gas & dust  Both young & older stars @ high density

88
Q

Halo

A

 No gas or dust or extremely rarified/tenuous & hot
 Mostly low mass, red, old stars
 Appears reddish/orange
 Globular clusters

89
Q

75~85% of large galaxies are

A

spiral or lenticular.

Very active galactic recycling

90
Q

Variations of spiral galaxies

Some have a bar of stars cutting
through their centres:

A

barred spiral galaxies  Spiral arms attached to ends of bar

91
Q

Latest data suggested Milky Way is a barred type

A

Its bulge appears elongated

92
Q

Others have NO spiral arms: Lenticular galaxies

A

 Uniform disk → looks like a lens seen edge-on

 Contain less cool gas than normal spiral galaxies

93
Q

Only spheroidal components, NO surrounding disk component.

A

 They are NOT globular clusters!

 Much more random star motion than orderly rotational one

94
Q

Elliptical galaxies Very little ISM, mostly low-density, hot

& ionized.

A

 Most ellipticals lack cool gas → little or no star formation
 Some have some cold gas & dust, e.g. as disks rotating around their centers
 Some large ellipticals have a lot of very hot gas  X-ray emission

Mostly cool stars, NO hot blue stars  look reddish/orange.
 Hence very little and slow galactic recycling, or none at all!!

95
Q

Elliptical galaxies  Very numerous, and have a very wide range of sizes

A

 The most massive galaxies are giant elliptical galaxies
 ~15% of all large galaxies are ellipticals  Vast majority of ellipticals are small → small elliptical galaxies are the most common type of galaxy in the Universe!

96
Q

Irregular galaxies

A
Miscellaneous class of galaxies. 
Appear white & dusty from ISM, like the disk of spirals
  Most are small & faint
 Contain young massive stars 
 Stars & gas clouds in random patches 
 Hence very active galactic recycling 

More likely to be distant galaxies
 Indicate they were more common when universe was young
 Milky Way’s close companions, the LMC & SMC are irregular galaxies

97
Q

Edwin Hubble invented a system for classifying galaxies

A

 The so-called “Hubble Tuning Fork”
 Classification made according to shape: It is NOT an evolutionary
sequence

98
Q

The number after “E” is

A

= 10((D-d)/D)

In 1959 de Vaucouleurs modified it into a more detailed classification system

99
Q

Many galaxies are not alone

A

gravitationally bound to other neighbours

100
Q

Galaxies often stay in loose collections of up to a few dozen called

A

groups

101
Q

The Milky Way is a relatively large galaxy, part of our

Local Group of galaxies

A

 3 m l.y. in size; ~40 galaxies  Within our Local Group → 2 large spirals: The Milky Way & the Andromeda galaxy (M31), the only one comparable in size

102
Q

Some galaxies associate in tightly bound clusters

.

A

 Contain 100s to 1000s galaxies over >10 m l.y.  Half of the large galaxies in clusters are elliptical

103
Q

The Local Group is part of the

A

Virgo supercluster

104
Q

Distance can be measured if we know the

A

apparent brightness & luminosity.

From parallax method on nearby stars

105
Q

Any astronomical object of known luminosity

A

is a standard candle.  IF we can find out its luminosity without first knowing its distance ! → e.g. any Sun-like star!

106
Q

Distance to standard candle can be determined by the inverse square law

A

 We only need to measure its apparent brightness (A.B.)

 However, Sun-like stars are dim at distances >1 kl.y.

107
Q

Key challenge to measure larger distances:

A

find better
(brighter) standard candles.

Luminosities of all main sequence stars are known
 use bright main sequence stars as standard candles:
 Distance to a close reference star cluster determined from parallax
 Plot its stars on the H-R diagram
 Measure relative brightness of unknown cluster
Determine distance to unknown cluster by comparing A.B. to known cluster

108
Q

Cepheid Variables & white dwarf supernovae

A

Cepheid variable stars → more luminous standard candles
 Bright giants → luminous enough to see at great distances
Follow well-defined period-luminosity relationships.
 Measuring period of variability tells us the luminosity (within 10%) With them we can measure distances up to 100 m l.y.! Very bright standard candles needed to measure intergalactic distances beyond the Milky Way.

109
Q

White dwarf supernovae (Type Ia) are distant standard candles.

A

All have same peak luminosity of 10 b Suns → Can be seen in galaxies b of l.y. away
 Calibrate those in nearby galaxies with Cepheids
 Must observe & measure when one explodes
 Not easily applicable: a white dwarf supernova (Type Ia) occurs only once every few hundred years in a typical galaxy

110
Q

The Tully-Fisher relation

A

Mass of spiral galaxy determines its rotation rate & luminosity → Luminosity-Rotation rate = a proportional dependence: L ∝ Vrot , with γ ≅ 4 but depends on wavelength λ thus Faster rotating spirals are more luminous
 Measure the 21 cm emission line of H gas in spiral disk with radio telescopes
 Compare Doppler shifts of portions of disk rotation towards us & away from us

111
Q

solar system

A

-4 ly (im gonna be saying in powers of 10)

112
Q

nearby stars

A

2

113
Q

milky way

A

5

114
Q

nearby galaxies

A

7

115
Q

galaxy clusters

A

10

116
Q

least to most accurate measuring methods

A

radar ranging > parallax > main-sequence-fitting > cepheids >distance standards

Chain of methods to measure size of universe.

117
Q

Edwin Hubble

A

Developed galaxy classification scheme. Studied stars in Andromeda galaxy and determined they were not in the Milky Way.
Also measured distances to other galaxies
 Measured the redshifts of distant galaxies
 discovered that more distant galaxies are moving faster away  The Universe is expanding

118
Q

Hubble’s Law:

A

The more distant a galaxy, the greater its redshift, and hence the faster it moves away from us

119
Q

Velocity-distance relation given by:

A

v = H0 . d
H0 = Hubble’s constant
 Often used to estimate galaxy’s distance from its redshift

120
Q

Hubble’s constant

A

Hubble’s constant is extracted from the velocity-distance plot of many galaxies.

121
Q

2 difficulties when trying to use practically Hubble’s law:

A

Galaxies do not obey Hubble’s law perfectly .  Gravitational influences from other neighbours alter their speeds.

122
Q

Distance determined from Hubble’s Law only as accurate as our best measurement of H0

A

20~24 km/s per m l.y. estimated by HST (~70…80 km/s/Mpc).

123
Q

What does it mean actually that the Universe is expanding 

A

The expansion of the Universe is the expansion of the SPACE ITSELF

Galaxies move apart with it but do not extend → gravity holds them together

124
Q

On very large scales, the distribution of galaxies is relatively uniform

A

 The overall appearance of the Universe is about the same no matter where you look or where you are located  No centre or edge

125
Q

COSMOLOGICAL PRINCIPLE =

A

the Universe is

uniformly distributed, without a center or an edge

126
Q

From any galaxy’s view,

A

other galaxies are all moving away from it. Galaxies must have been closer together in the past  The Universe must have a starting point!

127
Q

When did the Universe begin?

A

Run clock backward to starting point to determine age.
 Expansion rate assumed to be constant  Ho gives the rate galaxies are moving away from each another  1/Ho tells us how long it took to expand to current size → AGE!

128
Q

H0 = 22 km/s per m l.y. 

A

Age of universe, 1/H0 = 13.6 b years

129
Q

H0 = 21.8 km/s per m l.y. 

A

Age of universe, 1/H0 = 13.75 b years  Best available evidence indicates the Universe is ~14 b years old

130
Q

Ho changes with time but stays roughly equal to

A

1/(AGE of the Universe)

131
Q

Speed of light is finite

A

Light from galaxy 400 m l.y. away took 400 m years to arriv

132
Q

The relationship between distance, expansion & look-back tim

A

spacetime diagram

133
Q

How do we define the distance to a faraway galaxy?

A

 Is it distance when photons were emitted or are received?
Makes more sense to call this ‘the look-back time’.
 No ambiguity that photons took 400 m years to get here!

134
Q

Cosmological redshif

A

The shift to longer, redder wavelengths due to the expansion of the Universe which stretches out all the photons within it

 It tells us how much space has expanded during the time since light from the galaxy left on its journey to us

135
Q

Horizon of the Universe

A

aUniverse has no edge, but it does have a horizon.
 A place beyond which we cannot see!
Cosmological horizon = the place where the look-back
time equals the AGE of the Universe.
 Boundary in time, not in space
 Beyond this horizon you will be trying to see a time before
universe even existed!
 Observable universe grows
1 l.y. in size every year

136
Q

How did galaxies form?

A

Theoretical modeling must be used to study the earliest stage of galaxy life & evolution → assumptions:
H & He filled the space in the early Universe ( ≤ 1 m years )
 Matter was not uniformly distributed
We can see galaxies 13 b l.y. away (same age as oldest stars in Milky Way)
 most galaxies began to form at that time & have same age

137
Q

How did galaxies form? 2

A

The denser regions in the early Universe formed protogalactic clouds → cooled, contracted & collapsed to form galaxies.  The origin of the density enhancements in the early Universe is still a major unknown

 First-generation stars = massive   Supernovae → provided heavy elements and generated shock waves which heated up ISM   Slowed down collapse of protogalactic clouds & rate of star formation   Allowed gas to settle into a rotating DISK

138
Q

Why do galaxies differ?Differences between population of stars between the
galactic regions:

A

 Disk population → born AFTER the gas settled in a rotating disk (in a flat plane)  Spheroidal population → born BEFORE the gas settled in a rotating disk, hence with randomly oriented orbits around the center

139
Q

Distinct differences between S, E & Irr types of galaxies

A

→ their evolutions/lives are different: WHY? → 2 possibilities:

 Different ‘birth’ conditions in their protogalactic clouds  Similar formation but different evolutions due to interactions with other galaxies

140
Q

Galaxy formation 1) Conditions in the protogalactic cloud

A

1.1- Protogalactic spin:
 Significant amount of angular momentum = fast spin 
Spiral galaxy  Little or no angular momentum = slow (or no) spin  Elliptical galaxy

141
Q

Galaxy formation 1) Conditions in the protogalactic cloud 1.2- Protogalactic density

A

 Significant initial density → efficient energy radiation → quick cooling → fast star formation
 Elliptical galaxy  Low initial density → slow energy radiation → slow cooling → slow star formation  Spiral galaxy

142
Q

Galaxy evolution

A

Galaxies rarely evolve in perfect isolation Matter in Universe is constantly moving; even the Universe itself is constantly expanding
 Average distances between galaxies are not much larger than the sizes of galaxies 
COLLISIONS between galaxies are inevitable!

143
Q

Galaxy collisions were much more frequent in the past:

A

 Universe was smaller, matter denser, galaxies closer
 Protogalactic clouds collisions also must have happened
 Very spectacular but very slow events → 100s of m of years!
Distorted galaxies were more common in the early Universe

144
Q

When 2 spiral galaxies collide  Elliptical galaxy :

A

Tremendous tidal forces tear apart the disks → randomized orbits of the stars in long tails during first pass
 A large volume of their ISMs collapses at the center of collision
 rapid formation of new stars → Supernovae & stellar winds blow away remaining gas
 Ultimately, they form a single elliptical galaxy

Our galaxy will most likely merge with the Andromeda galaxy in 3 b years.

145
Q

Galaxies in dense clusters

A

At least some elliptical galaxies result from collisions & mergers
Ellipticals dominate the populations at the cores of dense clusters of galaxies → frequent collisions

146
Q

Central dominant galaxies = giant ellipticals at the center of many dense clusters :

A

Grew to huge sizes by consuming other galaxies  Frequently contain tightly bound clumps of stars → centers of the consumed galaxies

147
Q

Dense Clusters Very hot gas in the center of such dense clusters:

A

 Exerts a drag force on a spiral galaxy that may collide with it
  The spiral’s gas is slowed down, but the stars keep moving
  If the spiral’s disk had NOT previously formed many stars → the galaxy becomes an elliptical
 If the disk had already produced many stars BEFORE its gas was stripped out during the merger → becomes lenticular

148
Q

What are starbursts? L11  Starburst galaxies = galaxies in present-day Universe in which stars are forming at very rapid rates

A

 Milky Way → ~1 star per year  will not exhaust its ISM until long after the Sun died
 Starburst galaxies → >100 stars per year !  will consume ALL their ISM in a few 100s m years!

149
Q

Starburst galaxies

A

very bright in IR because of their ISM excited from UV & X-rays emitted from the many hot & young stars in it = so-called Ultraluminous Infrared Galaxies (ULRIGs)
 Starburst could be a phase in the evolution of a galaxy

150
Q

Starbursts explain why ellipticals lack

A

young stars & cool gas

151
Q

Causes of small-scale starbursts are

A

not clear

152
Q

Recent studies → collisions & mergers of gas-rich galaxies could

A

also cause starbursts

153
Q

What are starbursts?

A

A star formation 100 × faster than that of Milky Way  Supernovae will also occur 100 × more often!

 Supernovae generate a strong shock wave that creates a bubble of gas
 Shock waves from nearby supernovae overlap superbubble
 Further supernovae add more gas and thermal & kinetic energy

154
Q

When the superbubble breaks out of the galactic disk →

A

it will expand even faster & erupt into intergalactic space  galactic wind  It can blow the gas out of small galaxies  shut down star formation for many b of years in those galaxies

155
Q

Seyfert galaxies = one of the two largest groups of active galaxies, along with quasars

A

First described by Carl Seyfert in 1943.  10% of all galaxies; ~1% of all spirals.  Very few Seyfert galaxies are ellipticals.

156
Q

In visible, most Seyfert galaxies look like normal

A

normal spiral galaxies.  In other wavelength ranges, the luminosity of their cores is comparable to that of a whole galaxy the size of the Milky Way!

157
Q

Seyfert

A

They have quasar-like nuclei.

158
Q

Active galaxy

A

Active galaxy = A galaxy hosting an AGN 
AGN = An active galactic nucleus (AGN) is a compact region at the centre of a galaxy that has a much higher than normal luminosity over at least some portion, and possibly ALL, of the EM spectrum.
 The radiation from AGN is believed to be a result of accretion of mass by a supermassive black hole (SMBH) at the centre of its host galaxy

159
Q

The brightest AGNs are known as quasars

A

“ Quasi-stellar radio sources” = quasars
 The most powerful produce more light than 1,000 galaxies like the Milky Way!
 Observed only for very distant galaxies 
 Another temporary stage in the EARLY evolutions of galaxies → were most common b of years ago  Not seen nearby  objects that shine as quasars become dormant as galaxies age

160
Q

The incredible luminosities of quasars & AGNs are generated in a

A

volume not much bigger than our Solar system!

161
Q

We do NOT know much about their formation & lives,

A

and their link to the galaxies evolution

162
Q

Certain galaxies emit unusually strong radio waves  called radio galaxies

A

Much of the radiation does not come from the galaxy itself but from pairs of huge lobes, on each side of the galaxy  A strong AGN is hosted → drives 2 jets of particles streaming out at nearly the speed of light
 The jets hit ISM & intergalactic gas & excite it  radio hotspots
 The particles are then deflected & scattered → form the lobes

163
Q

What is the power source for quasars & AGNs ?L

A

Accretion of mass by a supermassive black hole (SMBH) at the centre of its host galaxy

164
Q

Accretion of mass by a supermassive black hole (SMBH) at the

centre of its host galaxy

A

Matter falling towards BH (up to relativistic velocities!) → Gravitational potential energy is converted into kinetic energy → Collisions & friction convert it into thermal energy  excitation of matter  intense radiation in a broad spectrum

 10…40% of the mass is converted into energy (Fusion: only 1% conversion efficiency!)

165
Q

What is the power source for quasars & AGNs ?

A

Accretion of mass by a supermassive black hole (SMBH) at the
centre of its host galaxy

Powerful jets due to twisted magnetic field

Same objects but viewed differently ! → Quasars & radio galaxies are THE SAME objects viewed in different ways

166
Q

power source for quasars & AGNs ?

Powerful jets due to twisted magnetic field

A

 Magnetic field lines twisted as accretion disk spins  Charged particles fly out along field lines into space

167
Q

power source for quasars & AGNs ?

Same objects but viewed differently ! → Quasars & radio galaxies are THE SAME objects viewed in different ways

A

When we can see directly the bright AGN → quasars  When dust obscures the bright AGN → radio galaxies

168
Q

We do NOT know why quasars eventually stop

A

shining so brightly or how they formed in the first place → linked to the SMBH formation
 We infer the existence of SMBHs from their influence on their surroundings
 Present evidence indicate that SMBHs are quite common

169
Q

The central supermassive black hole (SMBH) → closely related to the:

A

Galaxy’s spheroidal component: its mass MSMBH = MBulge/500

Spread σ of orbital velocities of the galaxy’s stars: MSMBH ∝ σ 4

170
Q

 The central BH growth is intrinsically linked with the

A

evolution of the galaxy

171
Q

Quasars & the study of intergalactic gas

A

 The formation & development of protogalactic clouds and their evolution into galaxies is not yet observed directly  Quasar spectra contains valuable info about the hydrogen clouds in the early Universe

172
Q

 Youngest galaxies observed to be made mostly of gas:

A

same mass in gas clouds as older galaxies have in the form of stars  Absorption lines from heavy elements seen only in mature galaxies

173
Q

We do NOT fully know yet how this process works! (supermassive black holes)
→ hints:

A

 SMBHs could result from the collisions of galaxies/protogalactic clouds
 Galaxies in the past were closer together/denser → more common collisions
 Galaxies in the past had more gas (not yet incorporated into stars)  feeding frenzy for the central BH!