Download presentation
Presentation is loading. Please wait.
1
The Milky Way PHYS390 Astrophysics Professor Lee Carkner Lecture 19
2
The Milky Way We can see the band of the Milky Way on a dark night Nature of galaxy not known until early 20 th century Basic structure Central dense bulge Old halo with dark matter
3
Disk Most visible area of the MW Diameter Sun is ~8 kpc from center Two components Thin disk of younger stars Site of current star formation Thick disk of older stars Fainter and has fewer stars (few % of thin disk)
4
Metallicity We use metal abundance as a proxy for age Normally use the iron to hydrogen ratio compared to the sun [Fe/H] = log [(N Fe /N H ) star / (N Fe /N H ) sun ] Range: -- 0 (exactly like the sun) Not perfectly reliable Iron comes from Type Ia supernovae and may vary with region Not completely mixed
5
Age of Disk Thin disk has broad range of metallicities Started forming stars 8 Gya and still going on today -0.6 to -0.4 Formed from episode of star formation between 10 and 11 Gya
6
Spiral Arms Gas, dust, young stars, bright stars, blue stars all concentrated in arms Hard to map in our galaxy Form via density waves As clouds orbit the Milky Way, they get stuck in areas of greater density
7
The Bulge The central part of the MW is a thickened bar-shaped bulge Hard for us to see due to extinction Due to several waves of star formation Region within which ½ of the light is emitted
8
Halo Above and below the disk are the globular clusters About 150 total Metallicity around -0.8 May be associated with thick disk Or else would have broken up over the last ~12 Gyr
9
Rotation Curve period of sun ~ 230 million years Luminous mass looks concentrated at the core Instead galaxy has flat rotation curve Rotational velocity constant with increasing distance from center
10
Dark Matter However, orbits of stars exterior to the sun indicate that there must be a total of about 10 12 M sun Dark matter is about 95% of total galactic mass Cannot be dust, gas or stars
11
Mass to Light Ratio of mass in solar masses to light in solar luminosities For total Milky Way ~ 60
12
Dark Matter Candidates MACHOs White dwarfs, neutron stars, black holes, red dwarfs, brown dwarfs Not enough detected in microlensing surveys WIMPs Weakly Interacting Massive Particles Should be able to detect in very large isolated detector arrays
13
Galactic Center Galactic center is 8 kpc from the sun in the constellation of Sagittarius Can find from distribution of halo globular clusters Best data from radio, IR and X-ray (not visible) stars are “isothermal”
14
Radio Observations A complex series of thermal and non-thermal sources At the center is a very bright, unresolved source, Sgr A* Less than ~2 AU in size
15
X-ray Observations Sgr A* corresponds to a bright X-ray source Explosions of material must have occurred in the past
16
IR Observations The K band at 2.2 m is used to observe stars close to Sgr A* Can use Kepler’s third law to find mass of Sgr A*
17
The Core Sgr A* has a mass of 3.7X10 6 M sun in a space less than 2 AU in size Destroys near-by stars to provide mass for accretion disk and outflows Black hole is fairly quiescent
18
Next Time Read 25.1-25.4 Homework: 24.2, 24.30, 24.33, 25.2b, 25.8a, 25.8b
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.