Plasma turbulence in tokamaks: some basic facts - PowerPoint PPT Presentation

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Plasma turbulence in tokamaks: some basic facts

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Applied Science: community ... MCF: Closed B-field lines, toroidal geometry ... these edge localized modes (ELMs) eject particles and energy on transit time ... – PowerPoint PPT presentation

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Title: Plasma turbulence in tokamaks: some basic facts


1
Plasma turbulence in tokamaks some basic facts
  • W.Fundamenski
  • UKAEA/JET

2
Controlled Nuclear Fusion
  • Applied Science community with a mandate
  • Goal Artificial Star on Earth, i.e. exo-thermal
    reactor
  • No gravity Magnetic (MCF) vs. Inertial (ICF)
    Confinement
  • MCF Closed B-field lines, toroidal geometry
  • Tokamak strong toroidal field, with weaker
    poloidal transform, hence net Helical field
  • Today JET, AUG, JT-60, DIII-D, MAST, NSTX,
  • Tomorrow ITER, a burning plasma experiment (EU,
    Japan, Korea, China, Russia, Canada, US)
  • Decision on site in final stages, expected by
    end of the year

3
Tokamaks I
  • Excellent textbook by J.Wesson,
  • eg. JET (Joint European Torus) near Oxford, UK
  • Core fields Btor ? 3 T, Edge Bpol ? 1 T ? 10,000
    Gauss
  • Core temperatures Ti,Te ? 10 keV, Edge Ti,Te ?
    100 eV
  • Core density ni,ne ? 1e20 m-3, Edge ni,ne ?
    1e19m-3
  • Low beta plasma, ß p_plasma / p_B lt 3
  • Btor ? 1/R, Bpol(jtor), poloidal transform
    necessary to prevent free (hoop) expansion via
    ExB drift

4
Tokamaks II
  • Core closed field lines, radial transport
  • Edge or SOL open field lines, parallel gtgt
    radial transport
  • Energy source neutral beams, ICRH, ECRH (in
    ITER and beyond fusion reactions themselves) heat
    the core
  • Particle source edge recycling gtgt core fuelling
  • Hence, mostly interested in power flow across
    B-field
  • Due to high temperatures, the core is very
    difficult to diagnose for fluctuations
  • Must rely on global transport reconstruction, to
    extract radial velocities, diffusivities,
    viscosities, conductivites, etc.
  • In the colder edge, some measurements are
    possible

5
Tokamaks III
  • Core transport found gtgt classical (Spitzer,
    Braginskii)
  • Also gtgt neo-classical (corrections for toroidal
    geometry)
  • Must infer the flow is not laminar but turbulent
  • Electrostatic vs. Electromagnetic turbulence
  • Comparison with theory suggests ion (critical
    gradient modes) dominate
  • 3-D Numerical codes (gyro-fluid and
    gyro-kinetic) are reaching a stage where global
    turbulence resolved
  • Transport barriers (local reduction of transport
    to laminar, neo-classical levels)
  • Edge (ETB) vs. internal (ITB) transport barriers
  • ETB L-H bifurcation, highly intermittent MHD
    bursts
  • these edge localized modes (ELMs) eject
    particles and energy on transit time scales
    similarity to solar flares ?!
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