UNH MURI Workshop: Planned Numerical Experiments - PowerPoint PPT Presentation

1 / 7
About This Presentation
Title:

UNH MURI Workshop: Planned Numerical Experiments

Description:

computational domain is 3-d non-periodic box with high b = 10? ... flow should have non-zero vorticity, to ensure some component of magnetic ... – PowerPoint PPT presentation

Number of Views:18
Avg rating:3.0/5.0
Slides: 8
Provided by: valued86
Category:

less

Transcript and Presenter's Notes

Title: UNH MURI Workshop: Planned Numerical Experiments


1
UNH MURI Workshop Planned Numerical Experiments
  • 3-d Emerged Bipole Form flux-rope in simulated
    corona by converging footpoints of coronal
    fields.
  • computational domain is 3-d non-periodic box with
    high b 10?) on bottom boundary,
    w/stratification such that b ltlt 1 within lower
    part of simulation volume.
  • intial condition (IC) has volume-filling dipole
    field.
  • impose incompressible converging flows on bottom
    boundary .

2
3d emeged bipole (contd)
  • initial magnetic field ought to be sheared, such
    that some component of the magnetic field is
    parallel to the magnetic neutral line at the
    bottom boundary or
  • if initial magnetic field is unsheared
    (potential?), imposed flow should have non-zero
    vorticity, to ensure some component of magnetic
    field is tangential to the magnetic neutral line
    on the bottom boundary
  • primary goal is to form flux rope subsequent
    efforts to erupt flux rope envisioned upon
    attainment of flux rope in corona
  • this experiment involves some modification of
    existing codes.
  • Critical issue 3-d necessary (no 2.5-d, or
    periodicity)

3
3-d Emerging Bipole
  • Flux rope in coronal volume via emergence of a
    pre-existing twisted flux tube from a region of
    high b to low b
  • IC buoyantly unstable horizontal twisted flux
    tube immersed in high-b plasma at base of
    gravitationally stratified 3-d box.
  • Follow rise of twisted flux tube from deep in
    convection zone through photosphere into corona.
    Critical issue initial position of tube cannot
    be too near surface, as flux tube curvature
    matters.
  • Unspecified parameter degree of twist in
    emerging tube. Twist too high perhaps prevents
    mass drainage, hampering emergence twist too low
    does not give true flux rope in corona.

4
3d emerging bipole (contd)
  • Unspecified parameter Magnetic field
    configuration in corona prior to flux rope
    emergence. Intial runs w/field-free corona
    envisioned.
  • As above, primary goal is to get flux rope in
    corona subsequent efforts to attain eruption
    envisioned after attainment of primary.
  • As above, some modification of existing codes
    necessary.

5
Bipole emergence in 3d multi-polar field
  • Emerge one flux tube into into background
    magnetic field sheared arcade/flux rope
    formation by reconnection between emerging flux
    and pre-existing flux.

6
Bipole emergence in multi-polar field (contd)
  • IC buoyantly unstable flux tube immersed in
    high-b plasma at base of gravitationally
    stratified 3-d box with background magnetic field
    configuration composed of a pre-emerged flux tube
    and large scale "restraining field," and form
    sheared arcade/flux rope by reconnection between
    the two flux tubes.
  • Critical issue without restraining field,
    reconnected flux expected to rise to top of
    computational volume in non-explosive manner.

7
Bipole emergence in multi-polar field (contd)
  • Primary goal is attainment of sheared arcade/flux
    rope in corona subsequent effort to attain
    eruption envisioned.
  • In one effort to attain eruption, additional
    polarity will be added to restraining field to
    make it quadrupolar.
  • Unspecified parameter twist in either
    pre-emerged or newly-emerging flux ropes.
    Presence of twist might either enhance or
    diminish storage of energy in the field, and
    hence likelihood of eruption.
Write a Comment
User Comments (0)
About PowerShow.com