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RUSSIAN ACADEMY OF SCIENCES KELDYSH INSTITUTE FOR APPLIED MATHEMATICS

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Large time scales ideal MHD numerical simulation of the magnetic field loop ... At outer boundary R=Rout incoming wave strengths vanish ... – PowerPoint PPT presentation

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Title: RUSSIAN ACADEMY OF SCIENCES KELDYSH INSTITUTE FOR APPLIED MATHEMATICS


1
RUSSIAN ACADEMY OF SCIENCES KELDYSH INSTITUTE
FOR APPLIED MATHEMATICS
  • NUMERICAL SIMULATION OF THE MAGNETIC FIELD
  • CORONAL LOOP EVOLUTION
  • Tatiana Yelenina
  • 2006

2
  • Purpose
  • Large time scales ideal MHD numerical simulation
    of the magnetic field loop evolution in the
    ''star disk'' system
  • Topics under consideration
  • Construction and verification of the high
    resolution scheme for the ideal MHD equations
  • Investigation of the main features of the
    star-disk system evolution scenario

'Star disk'' system
3
Scheme for 2D MHD equations
  • Finite volume method
  • Godunov type scheme, approximate Riemann solver
  • To guarantee divergence-free magnetic field
    through the vector potential
  • Explicit approximations of the forcing term

Tóth G.
4
''Star corona disk'' system
Star mass ?, angular velocity ?, magnetic
moment ?
Corona perfectly conducting plasma
Disk Keplerian infinitely thin (h lt cs/?kltlt r)
conducting plane consisted of the dense cold
matter (?s ltlt Vk) Disk surface electrical
conductivity ? c2 / (2? ?t cs), Disk
surface magnetic diffusivity ? c2 / (2? ?)
?tcs ?t(cs / Vk)Vk
Shakura-Sunyaev ? - disk model
5
Governing equations
Continuity equation
Momentum equation
Induction equation
Energy equation
div B 0
Tik ?vivk pdik BiBk /(4p) B2dik /(8p), g
-?Fg, Fg - GM / R, S p/ ??
6
Boundary conditions
  • In disk ? ? /2 ( v-Vk ) B? ( w ?
    ) Bf 0
  • uB? ( w ? ) Br 0
  • w ac vc2az2 / (c2 a2) 0
  • Sd const
  • At inner boundary RRin u V ef , B
    RRin 0, V O Rin sin ?
  • At outer boundary RRout incoming wave
    strengths vanish
  • On rotation axis flow symmetry conditions

Initial conditions
  • Stellar magnetic field (dipole-like topology,
    with magnetic moment ? ) penetrates the corona
    and the disk.
  • Corona and disk are in mechanical equilibrium
    with the force-free
  • dipole magnetic field.

7
Numerical simulation of the magnetic field
coronal loop evolution
  • Purpose of the numerical experiments
    investigation of
  • type of the system evolution steady state or
    periodic regime and its characteristics
  • intensity of angular momentum transport from
    the disk
  • disk surface magnetic diffusivity influence on
    the scenario of star-disk system evolution

8
Initial distribution of the entropy S(r,z) and
angular velocity ?(r,z)
9
Flow distribution at ? 0, t 50
10
Flow distribution at ? 0.001, t 50
11
Flow distribution at ? 0.005, t 50
12
Magnetic field topology dependence on the disk
surface magnetic diffusivity ?
13
Time dependence of the angular momentum fluxes on
the disk surface magnetic diffusivity ?
? 0
? 0.001
? 0.005
14
Electric current density and magnetic field lines
in corona
15
Conclusions
  • Magnetic field coronal loop evolution consists in
    periodic reconnection of the magnetic field lines
    and plasmoid ejections which yields to
    oscillations of the flux angular momentum taken
    away from the disk.
  • Intensity and periodicity of the process strongly
    depend on disk electrical conductivity.
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