Star Formation Dark Matter and Baryons Gravity (DM) defines large - - PowerPoint PPT Presentation
Star Formation Dark Matter and Baryons Gravity (DM) defines large - - PowerPoint PPT Presentation
Star Formation Dark Matter and Baryons Gravity (DM) defines large scale structure of the Universe Baryons are mostly hitchhiking a ride Yet, their physical interactions are far richer Gastrophysics How are stars
KAS16/MT Lecture1II - Star Formation
2
Dark Matter and Baryons
★Gravity (DM) defines
large scale structure of the Universe
★Baryons are mostly
hitchhiking a ride
★Yet, their physical
interactions are far richer
★“Gastrophysics” ★How are stars formed?
KAS16/MT Lecture1II - Star Formation
3
KAS16/MT Lecture1II - Star Formation
4
KAS16/MT Lecture1II - Star Formation
5
KAS16/MT Lecture1II - Star Formation
6
KAS16/MT Lecture1II - Star Formation
7
KAS16/MT Lecture1II - Star Formation
8
KAS16/MT Lecture1II - Star Formation
9
KAS16/MT Lecture1II - Star Formation
10
KAS16/MT Lecture1II - Star Formation
11
KAS16/MT Lecture1II - Star Formation
12
KAS16/MT Lecture1II - Star Formation
13
KAS16/MT Lecture1II - Star Formation
14
KAS16/MT Lecture1II - Star Formation
15
KAS16/MT Lecture1II - Star Formation
16
KAS16/MT Lecture1II - Star Formation
17
KAS16/MT Lecture1II - Star Formation
18
★ Gas in the Interstellar Medium is not dense enough
KAS16/MT Lecture1II - Star Formation
19
Radiative cooling
★How do you expect cooling to depend
- n metallicity of gas?
KAS16/MT Lecture1II - Star Formation
20
Radiative cooling and “metals”
★ Simple atoms and molecules are inefficient at
radiative cooling
★ Metal-free gas (Z<10-3.5ZSun) hard to cool ★ The more “metals” the more efficient the cooling:
many energy levels available
★What is your expectation for the Jeans mass in
first gas clouds?
KAS16/MT Lecture1II - Star Formation
21
Log{Cooling efficiency}
★ But cooling
efficiency grows with temperature
KAS16/MT Lecture1II - Star Formation
22
Log{Cooling efficiency}
★ But cooling
efficiency grows with temperature
★ WHY?
KAS16/MT Lecture1II - Star Formation
23
DM halos and cooling of gas
★ Temperature of gas in DM halos depends on halo
mass and redshift
★There is a minimum halo mass for which cooling is
efficient (cooling time less than Hubble time)
KAS16/MT Lecture1II - Star Formation
24
Minimum halo for cooling
Trenti & Stiavelli (2009)
z Mcool Tvir=1e4K minimum halo mass for cooling
KAS16/MT Lecture1II - Star Formation
25
Gas cloud starts to contract
It gets smaller and denser And smaller...
Denser, Hotter until H-fusion begins: A star is born!
The simple picture
KAS16/MT Lecture1II - Star Formation
26
KAS16/MT Lecture1II - Star Formation
27
KAS16/MT Lecture1II - Star Formation
28
KAS16/MT Lecture1II - Star Formation
29
KAS16/MT Lecture1II - Star Formation
30 Smith et al. (2009) n [cm-3] T [K]
KAS16/MT Lecture1II - Star Formation
31
KAS16/MT Lecture1II - Star Formation
32
KAS16/MT Lecture1II - Star Formation
33