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BOUT

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Points to a problem with the kink/peeling drive (sensitive to plasma-vacuum boundary) ... compare non-linear evolution with and without kink-component ... – PowerPoint PPT presentation

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Title: BOUT


1
BOUT Towards an MHD Simulation of ELMs
  • B. Dudson and H.R. Wilson
  • Department of Physics, University of York
  • M.Umansky and X.Xu
  • Lawrence Livermore National Laboratory, CA
  • P.Snyder
  • General Atomics, San Diego, CA

2
Outline
  • BOUT motivation and philosophy
  • ELM modelling the approach and objectives
  • Initial benchmarking results (work in progress),
    and future aims

3
BOUT Philosophy
  • BOUT is a collaborative project between
    University of York and LLNL
  • The code provides a framework for developing
    plasma fluid codes
  • user defined magnetic geometry (in terms of
    metrics)
  • user-defined plasma model
  • Flexible, user-friendly code (small compromise
    on speed)
  • easy to adjust plasma physics model, and explore
    implications

4
Example of the code Ideal MHD equations
dndt -nDiv(v) V_dot_Grad(v,n)
dpdt V_dot_Grad(v,p) - gammapDiv(v)
dvdt V_dot_Grad(v,v) ((Curl(B)B) -
Grad(p))/n
dBdt Curl(vB)
5
Physics Objectives
  • There are two main objectives
  • Edge turbulence modelling
  • Edge MHD and ELMs
  • focus on the ELM modelling here

6
ELM modelling- the approach
  • Two complementary approaches to tackle the ELM
    problem
  • Full non-ideal MHD code, towards a model for the
    ELM crash
  • A range of codes being used NIMROD, BOUT,
    JOREK, M3D, etc
  • Advantage well-developed codes, some with
    2-fluid effects
  • Disadvantage difficult to pull out and and
    study the impact of specific physics elements
    without a detailed knowledge of the code making
    contact with analytic theory is not easy
  • Building up from simple ideal MHD model
  • Basic ideal MHD model eases comparison with
    analytic theory and linear codes (eg ELITE and
    non-linear ballooning theory)
  • The model can then be slowly built up,
    monitoring the impact of different physics
    effects
  • BOUT is ideally suited to exploring the second
    approach
  • permits the user to add and subtract physics in
    a clear way

7
Initial benchmark studies (in progress)
  • The Orszag-Tang vortex provides a standard
    test of 2D ideal MHD solvers looks good,
    qualitatively
  • Tests the ability to treat shocks (possibly
    important for ELMs)

Athena, Roe solver
BOUT, ideal MHD
8
Quantitative Benchmark linear ideal MHD
  • We have begun to test the code against ELITE
  • For initial tests, we have implemented a reduced
    ideal MHD model into BOUT
  • Valid for high-n ballooning modes
  • Initial case strong instability, with
    significant peeling component
  • OK for intermediate n, but unable to reproduce
    higher n (yet)
  • Points to a problem with the kink/peeling drive
    (sensitive to plasma-vacuum boundary)

9
Produces fingers in non-linear regime
  • Mode propagates radially
  • Filamentary structures are produced in the
    non-linear regime
  • Cannot take too seriously while there is
    disagreement in the linear regime
  • but encouraging first signs!

10
New equilibrium to minimise coupling to vacuum
  • Presently exploring a more ballooning case, with
    reduced coupling to vacuum (ELITE requires some
    edge interaction)
  • ELITE predicts close to marginal stability
    g/wA0.01

Equilibrium mesh
ELITE
11
The challenges of marginal stability
  • Agreement has not yet been achieved (the BOUT
    runs take 12 hours, while ELITE is 3 minutes, so
    comparisons are not trivial)
  • It is necessary to work close to linear marginal
    stability
  • it is the experimentally relevant situation (p
    increases slowly through marginal stability
  • modes that are strongly unstable linearly are
    likely to have different dynamics
  • existing non-linear theories are based on
    proximity to marginal stability
  • One issue with proximity to marginal stability
    is resolution of fine-scale structures near
    rational surfaces
  • makes sense to use nq as the radial variable to
    improve resolution around rational surfaces (pack
    mesh there) presently exploring this
  • When we go non-linear, an additional challenge
    will be the time taken to get into the non-linear
    regime
  • will need to make use of scaling of mode
    structure during linear phase to speed code up
    here

12
Future plans the strategy
  • Work to find a mesh and formalism that gives
    agreement with ELITE close to marginal stability
    with weak coupling to vacuum
  • Extend/return to linear tests where mode couples
    to vacuum
  • Extend to non-linear regime
  • compare non-linear evolution with and without
    kink-component
  • Extend to include non-ideal physics (care
    unphysical modes can be introduced when
    dissipation is introduceddiamagnetic effects
    will be an important first effect to include).
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