SLIDE 1 Stars + Galaxies: Back of the Envelope Properties
David Spergel
SLIDE 2 Free-fall time
(1) ¨ r = −GM r2 (2) r t2 = −GM r2 (3) tfree−fall ≃ r3 GM ≃ 1 √Gρ Free-fall time for neutron star is milliseconds (char- acteristic timescale for gravitational waves) Free-fall time for the Sun is 103s (characteristic timescale for gravitational waves)
Characteristic time for universe = Hubble Time
SLIDE 3 Cosmology
˙ a a 2 = 8π 3 Gρ t−2 ∝ Gρ
SLIDE 4 Kelvin-Helmholtz Time
- Time scale to radiate gravitational energy
U = GM2/R t = GM2/RL 30 million years for the Sun Timescale for proto-star evolution
SLIDE 5 Einstein Time
- Time scale to radiate gravitational energy
U = Mc2 t = Mc2/L 1013 years for the Sun
SLIDE 6 Nuclear Energy Timescale
nucleon
- Sun doesn’t use all of the
available fuel
U = εMc2 t = εMc2/L
SLIDE 7 Nuclear Burning
R =
∝
2kT S(E) E exp Z1Z2e2 hv
SLIDE 8 Stellar Structure
- Hydrostatic Equilibrium:
- Mass Conservation:
- Thermal Conduction:
- Equation of State:
- Energy Production:
SLIDE 9 Hydrostatic Equilibrium
dp dR = −GM(r) R2 ρ Using ¯ ρ ≃ M∗/R3
∗, this implies
p∗ R∗ = GM∗ R2
∗
M∗R3
∗ = GM 2 ∗
R5
∗
Using ideal gas law, p = ρkT/µ, kT = GMµ R
SLIDE 10 Mass-Luminosity Relation
dT dR = − l(r) 4πr2 3 16 κρ σBT 3 Using ¯ ρ ≃ M∗/R3
∗, this implies
L = R2T 3
∗
ρ T∗ R∗ L ∝ M 3
∗
SLIDE 11
Mass Luminosity Relation
SLIDE 12 Stellar Lifetimes
t = ǫMc2 L t ∝ M −2 Massive Stars live short brilliant lives!
SLIDE 13 Stellar Populations
Mass function: dn dM ∝ M −2.35 The lowest mass stars dominate the mass of a stel- lar population L(t) = Mmax(t) M −2.35L(M)dM = M 2.15
max(t) ∝ t−1.07
The most massive stars dominate the luminosity
SLIDE 14 Radii and Temperature
R ∝ M 0.9 L ∝ T 4R2 T ∝ L0.25 R0.5 ∝ M 0.4
SLIDE 15
Spiral Arms
SLIDE 16 Later Stages of Stellar Evolution
- Red Giant Branch (RGB)
- Degenerate Core of Helium
- Envelope burning Hydrogen
- Helium Flash
- Horizontal Branch
- Core burning of Helium to Carbon
- Asymptotic Giant Branch (AGB)
- Degenerate Core of Carbon
- Envelope burning Helium
SLIDE 17 Fuel Consumption Thereom
The contribution by any Post Main Sequence evolutionary phase to the total luminosity of a simple stellar population is proportional to the amount of nuclear fuel burned in that phase
tHB tMS = LMS LHB UHB UMS ≃ LMS LHB EHe→C EH→He
SLIDE 18 Degeneracy Pressure
- As a star burns H -> He, it leaves behind a
degenerate gas supported by electron degeneracy pressure
- Nuclear burning cycles are alternated by
period of rapid gravitational collapse
- Chandrasekhar Mass (maximum mass
supported by degeneracy pressure) (followed by flashes)
SLIDE 19 Chandrasekhar Mass
EG = −GM 2 R When the electrons become relativistic, their total Fermi energy is approximately, EF = NcpF = Nc ∆x
R = M 4/3c m4/3
p R
Equating the two: Mch = c G 3/2 1 m2
p
= M 3
Pl
m2
p
SLIDE 20
HR Diagram
SLIDE 21
Globular Cluster HR Diagram
SLIDE 22
SLIDE 23 Stellar Models
- MESA (Paxton et al. 2011, ApJS, 192, 3)
- mesa.sourceforge.net
- Can stably evolve stars through Helium
flash, RGB and HB to White Dwarf
SLIDE 24 Dust and Gas
- Stars form in Molecular Clouds
- These clouds contain copious amounts of
dust that absorb starlight (in the optical, UV and near IR) and reemit in the IR
- Dust grains are micron size and composed
primarily of carbon and silicates
SLIDE 25 Dust Emission
- Electric Dipole Limit (Size << λ)
σabs ∝ λ−2 Fν ∝ ν2Bν(T) ∝ ν4
SLIDE 26
Galaxy Spectrum
SLIDE 27 Other Emission Processes
- Radio:
- Free-free emission
- Synchrotron emission
- Radio emission scales with synchrotron
SLIDE 28
X-ray UV VIS Radio Far IR Mid IR Near IR M81 D=3 Mpc
SLIDE 29 Galaxy Properties
David Spergel
SLIDE 30
SLIDE 31
Tinker et al. 2008
SLIDE 32
SLIDE 33
Blanton et al. 2002 4 Gyr burst
SLIDE 34
4000 Angstrom Break
SLIDE 35
SLIDE 36
Kauffmann et al. 2003
SLIDE 37
Galaxy Morphology
SLIDE 38 Spiral Galaxies
Sanders and Verheijen 1998
family: Luminosity and Surface Brightness
distribution of stars
SLIDE 39 Spiral Galaxy Formation
- Tidal torque generates solid body rotation
in gas
- Gas cools and collapses to form a disk
conserving angular momentum
SLIDE 40
SLIDE 41 Elliptical Galaxies
- Re effective radius
- Ie mean surface brightness
within eff. radius
log Dn = log Re + 0.8 log Ie
SLIDE 42
Black Hole Scaling Relation
Gultekin et al. 2009