| hot stars > Corotating Interaction Regions |
This page contains movies of hydrodynamical simulations
of Corotating Interaction Regions (CIRs).
In a radiatively driven
stellar wind, a bright spot on the surface creates a perturbance (a CIR) which
travels through the wind.
This CIR is seen as a spiral-shaped density
enhancement,
compared to the smooth wind. The CIR also perturbs the velocity field.
CIRs are responsible for the Discrete Absorption Components seen
in some ultraviolet resonance lines of hot stars.
This work has been published in Lobel & Blomme (2008, ApJ, 678, 408). Click here for the ADS link. Conference proceedings of this work can be found here and here .
This webpage concentrates on the hydrodynamics of the CIRs. Their relation to Discrete Absorption Components is discussed here.
All these simulations were made using the
Zeus3D
hydrodynamics code
(Stone
and Norman 1992).
The star and wind parameters are those of the B0.5 Ia star HD 64760.
| Effective temperature | = | 24 600 K |
| Luminosity | = | 1.55 x 105 solar |
| Radius | = | 22 solar radii |
| Mass | = | 20 solar masses |
| Terminal velocity | = | 1 500 km/s |
| Mass loss rate | = | 9 x 10-7 solar masses per year |
| Rotational velocity vrot | = | 265 km/s (assumes sin i = 1) |
Each movie comes in AVI and MP4 format.
The colour scale is used to show the density contrast with respect to
a smooth wind.
The velocity vectors are those with respect to a smooth wind. The length scale
of the velocity vectors can differ from one movie to the other.
Each movie shows two rotations of the CIR. All movies run at the same
"speed", but the real time taken for a spot pattern to rotate will depend
on the model.
one spot on the stellar surface
one spot on the stellar surface
Trace particles have been added to show their nearly-radial outflow
(except very close to the stellar surface where they rotate
due to angular momentum conservation).
The particles emitted at the centre of the CIR do not
remain in the CIR, but go through it.
The CIR is not a stream of particles, but a pattern in the wind.
A circle (centred on the star)
is drawn through the green point that started at the
centre of the CIR. This helps to see the
(small) velocity differences between
the different trace particles.
two spots on the stellar surface, each one
two different spots on the stellar surface, with
one spot on the stellar surface
one spot on the stellar surface
one dark spot on the stellar surface
four spots on the stellar surface, each one
AVI
MP4
A=0.10; Phi=50 degrees;
vspot=vrot/2.5; 1 rotation of spot=10.3 days
maximum density contrast=1.21
largest velocity vector=91 km/s
AVI
MP4
A=0.10; Phi=50 degrees;
vspot=vrot/2.5; 1 rotation of spot=10.3 days
AVI
MP4
A=0.20; Phi=20 degrees;
vspot=vrot/5; 1 rotation of spots=20.6 days
maximum density contrast=1.32
largest velocity vector=143 km/s
AVI
MP4
A=0.20; Phi=20 degrees, and
A=0.08; Phi=30 degrees;
vspot=vrot/5; 1 rotation of spots=20.6 days
maximum density contrast=1.32
largest velocity vector=143 km/s
AVI
MP4
A=0.50; Phi=180 degrees;
vspot=vrot/10; 1 rotation of spot=41.2 days
maximum density contrast=1.97
largest velocity vector=226 km/s
AVI
MP4
A=0.50; Phi=90 degrees;
vspot=vrot*3; 1 rotation of spot=1.373 days
maximum density contrast=2.07
largest velocity vector=180 km/s
AVI
MP4
A=-0.30; Phi=30 degrees;
vspot=vrot/2.5; 1 rotation of spot=10.3 days
maximum density contrast=1.53
largest velocity vector=380 km/s
AVI
MP4
A=0.10; Phi=30 degrees;
vspot=vrot/10; 1 rotation of spots=41.2 days
maximum density contrast=1.16
largest velocity vector=88 km/s