Magnetorotational instability in the solar core and Ap star envelopes - PowerPoint PPT Presentation

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Magnetorotational instability in the solar core and Ap star envelopes

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decay close-up. Rm = 104. Pm = 1. Ra = 0. Differential-rotation. decay close-up. Resolution at high Reynolds number. t = 1 rotation. t = 4 rotations ... – PowerPoint PPT presentation

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Title: Magnetorotational instability in the solar core and Ap star envelopes


1
Magneto-rotational instability in the solar core
and Ap star envelopes
  • Rainer ArltAstrophysikalisches Institut Potsdam
  • and Günther Rüdiger, Rainer Hollerbach

2
Solar rotational evolution
  • Wind model by Stepien (1988)

3
The solar tachocline and the core
  • Thompson et al. 2003 from various sources

4
Stellar radiative envelopes
  • Star of spectral type A and B
  • Small convective core
  • Extensive radiative zone
  • 10 of these starshave magnetic fields
  • These 10 are slowrotators

5
Differential-rotation decay
  • Rotation of solar core is slow and uniform
  • Rotation period has increased by factor of 10
    during life
  • Viscosity too small to reduce rotation
    homogeneously throughout the Sun
  • Magnetic Ap stars rotate much slower than
    normal A stars
  • Did MRI reduce the internal rotation of Sun and
    Ap stars?

6
Magneto-rotational instability
  • Angular velocity decreasing withaxis distance
  • Magnetic field or arbitrary geometry
  • Instability with growth rate of the order of ?

7
Lower limit for MRI
k of most un-stable mode depends on B Diffusive
decay rate increases with k ? MRI sup-pressed
below certain B
in Gauss
8
Upper limit for MRI
Wavelength of most un-stable MRI mode exceeds
object size
in kG
9
Numerical simulations
  • Spherical spectral code (Hollerbach 2000)

10
Initial conditions
  • Vertical cut through radiativezone
  • LeftMagnetic field
  • RightAngular velocity

11
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12
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13
Differential-rotationdecay close-up
Rm 104Pm 1Ra 0
14
Differential-rotationdecay close-up
15
Resolution at high Reynolds number
t 4 rotations
t 8 rotations
t 1 rotation
16
Resolution at high Reynolds number
t 4 rotations
t 1 rotation
t 8 rotations
17
Differential-rotation decay
  • Steepness of rotation profile versus time
  • Initially
  • Rayleigh-stable

18
Differential-rotation decay timeversus Reynolds
number
19
Effect of negative buoyancy
Rm 2104Pm 1Ra -108
20
Effect of negative buoyancy
21
Differential-rotation decay
  • Extrapolation to stellar parameters
  • Decay time of 10-100 million years
  • Short compared with the age of the Sun (5 billion
    years) ? MRI may have provided the enormous
    angular-momentum transport for slow-down
  • Considerable fraction of Ap star ages (life-time
    lt 109 yr) ? MRI may still beoperating in them.

22
The End
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