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Radiatively Driven Winds and Aspherical Mass Loss

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Radiatively Driven Winds and Aspherical Mass Loss. Stan Owocki. U. ... Joss, Salpeter Ostriker 1973. Photon tiring. Stagnation of photon-tired outflow. Shaviv ... – PowerPoint PPT presentation

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Title: Radiatively Driven Winds and Aspherical Mass Loss


1
Radiatively Driven Winds and Aspherical Mass Loss
Stan Owocki U. of Delaware
collaborators Ken Gayley U. Iowa Nir Shaviv
Hebrew U. Rich Townsend U. Delaware Asif
ud-Doula NCSU
2
General Themes
  • Lines vs. Continuum driving
  • Oblate vs. Prolate mass loss
  • Smooth vs. Porous medium
  • Rotation vs. Magnetic field

3
Radiative force
4
Line Scattering Bound Electron Resonance
for high Quality Line Resonance, cross section gtgt
electron scattering
5
Optically Thick Line-Absorption in an
Accelerating Stellar Wind
For strong, optically thick lines
6
CAK model of steady-state wind
Equation of motion
inertia
gravity
CAK line-force
Solve for
7
Wind Compressed Disk Model
Bjorkman Cassinelli 1993
8
Wind Compressed Disk Model
Bjorkman Cassinelli 1993
9
Wind Compressed Disk Simulations
radial forces only
10
Wind Compressed Disk Simulations
radial forces only
11
Vector Line-Force from Rotating Star
12
Gravity Darkening
increasing stellar rotation
13
Vector line-force With gravity dark.
14
Effect of gravity darkening on line-driven mass
flux
15
Rotational effect on flow speed

16
Smith et al. 2002
17
Smith et al. 2003
18
But lines cant explain eta Car mass loss
19
Super-Eddington Continuum-Driven Winds
moderated by porosity
20
Continuum Eddington parameter
constant in radius gt no surface modulation
21
Convective Instability
  • Classically expected in energy-generating core
  • e.g., CNO burning gt e T10-20 gt dT/dr gt
    dT/drad
  • But envelope also convective where G(r) -gt 1
  • e.g., z Pup G1/2 gt M(r) lt M/2 convective!
  • For high density interior gt convection efficient
  • Lconv gt Lrad - Lcrit gt Grad (r) lt 1
    hydrostatic equilibrium
  • Near surface, convection inefficient gt
    super-Eddington
  • but flow has M L/a2
  • implies wind energy Mvesc2 gtgt L
  • wouldtire radiation, stagnate outflow
  • suggests highly structured, chaotic surface

Joss, Salpeter Ostriker 1973
.
.
22
Photon tiring
23
Stagnation of photon-tired outflow
24
Shaviv 2001
25
Power-law porosity
26
Effective Opacity for "Blob"
27
Porous opacity
28
Super-Eddington Wind
Shaviv 98-02
  • Wind driven by continuum opacity in a porous
    medium when G gt1

At sonic point
porosity-length ansatz
29
Power-law porosity
Now at sonic point
30
Results for Power-law porosity model
31
Effect of gravity darkening on porosity-moderated
mass flux
32
Eta Carina
33
Summary Themes
  • Lines vs. Continuum driving
  • Oblate vs. Prolate mass loss
  • Smooth vs. Porous medium
  • Rotation vs. Magnetic field

34
Wind Magnetic Confinement
Ratio of magnetic to kinetic energy density
for Homunclus, need B104 Ggt
for present day eta Car wind, need B103 G
35
MHD Simulation of Wind Channeling
No Rotation
Confinement parameter
A. ud Doula PhD thesis 2002
36
Field aligned rotation
A. ud-Doula, Phd. Thesis 2002
37
Disk from Prograde NRP
w0.95 DVamp a 25 km/s DVorb
38
Azimuthal Averages vs. r, t
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