Transport and confinement in the Mega Ampère Spherical Tokamak (MAST) plasma

A combination of recently installed state-of-the-art imaging and profile diagnostics, together with established plasma simulation codes, are providing for the first time on Mega Ampere Spherical Tokamak (MAST) the tools required for studying confinement and transport, from the core through to the plasma edge and scrape-off-layer (SOL). The H-mode edge transport barrier is now routinely turned on and off using a combination of poloidally localized fuelling and fine balancing of the X-points. Theory, supported by experiment, indicates that the edge radial electric field and toroidal flow velocity (thought to play an important role in H-mode access) are largest if gas fuelling is concentrated at the inboard side. H-mode plasmas show predominantly type III ELM characteristics, with confinement HH factor (w.r.t. scaling law IPB98[y, 2]) around ~1.0. Combining MAST H-mode data with the International Tokamak Physics Activities (ITPA) analyses, results in an L–H power threshold scaling proportional to plasma surface area (rather than PLH ~ R2). In addition, MAST favours an inverse aspect ratio scaling PLH ~ e0.5. Similarly, the introduction of type III ELMing H-mode data to the pedestal energy regression analysis introduces a scaling Wped ~ e−2.13 and modifies the exponents on R, BT and κ. Preliminary TRANSP simulations indicate that ion and electron thermal diffusivities in ELMing H-mode approach the ion-neoclassical level in the half-radius region of the plasma with momentum diffusivity a few times lower. Linear flux-tube ITG and ETG microstability calculations using GS2 offer explanations for the near-neoclassical ion diffusivity and significantly anomalous electron diffusivity seen on MAST. To complement the baseline quasi-steady-state H-mode, newly developed advanced regimes are being explored. In particular, 'broad' internal transport barriers (ITBs) have been formed using techniques developed at conventional aspect ratio. Electron and ion energy diffusivities are reduced towards the ion-neoclassical level in the ITB region of both co- and counter-injection NBI heated plasmas, with momentum diffusivity up to 10 times lower. Moving out to the edge and SOL, OSM2/EIRENE modelling is being used to extract edge perpendicular particle and heat diffusivities, results being consistent with the ballooning nature of power-flow seen in L-mode and reduction in outboard turbulence seen in ELM-free and inter-ELM H-mode. Modelling of parallel SOL transport requires the inclusion of the mirror force (~10 times higher in MAST than at the conventional aspect ratio) and B2SOLPS5.0 simulations show the edge electric field to be well modelled by neoclassical theory. Transient edge transport phenomena are being studied in detail using a variety of techniques (e.g. probability density function (PDF) and power spectrum analysis, differencing and rescaling methods). Intermittent transport is associated with a radial efflux at up to a tenth of the sound speed and up to 30 cm from the separatrix. Arguably, the most dramatic edge events seen in the plasma periphery are the ELMs. Recent results using fast, high-resolution visible imaging confirm the hypothesis that ELMs have both poloidal and toroidal structures (n ~ 10 at q = 4), consistent with recent theories of the non-linear evolution of ballooning modes.

[1]  G. F. Counsell,et al.  ELM characteristics in MAST , 2004 .

[2]  I. Voitsekhovitch,et al.  Numerical Transport Codes , 2004 .

[3]  O. Sauter,et al.  Overview of recent experimental results on MAST , 2003 .

[4]  O. Hurricane,et al.  Explosive instabilities: from solar flares to edge localized modes in tokamaks , 2003 .

[5]  V. Gusev,et al.  The basics of spherical tokamaks and progress in European research , 2003 .

[6]  D. A. Gates,et al.  Progress towards high-performance, steady-state spherical torus. , 2003 .

[7]  J. G. Cordey,et al.  A two-term model of the confinement in Elmy H-modes using the global confinement and pedestal databases , 2003 .

[8]  W. Fundamenski,et al.  Parallel SOL transport in MAST and JET: the impact of the mirror force , 2003 .

[9]  C. Bourdelle,et al.  Stabilizing impact of high gradient of β on microturbulence , 2003 .

[10]  J. Breslau,et al.  Nonlinear simulation studies of tokamaks and STs , 2003 .

[11]  E. D. Fredrickson,et al.  Recent results from the National Spherical Torus Experiment , 2003 .

[12]  E. D. Fredrickson,et al.  β-Limiting MHD instabilities in improved-performance NSTX spherical torus plasmas , 2003 .

[13]  D. A. Gates,et al.  High β, long pulse, bootstrap sustained scenarios on the National Spherical Torus Experiment (NSTX) , 2003 .

[14]  K. Tritz,et al.  Performance and stability of near-unity aspect ratio plasmas in the Pegasus Toroidal Experiment , 2003 .

[15]  G. Counsell,et al.  Use of one dimensional Dα camera to measure edge electron density gradients , 2003 .

[16]  J. Ahn,et al.  A review of plasma boundary phenomena in the mega ampere spherical tokamak , 2003 .

[17]  J. Ahn,et al.  The influence of the divertor magnetic configuration and of ELM frequency on target heat fluxes in MAST , 2003 .

[18]  B. LaBombard,et al.  Universality of Intermittent Convective Transport in the Scrape‐off Layer of Magnetically Confined Devices , 2003 .

[19]  A. Becoulet,et al.  Hot spot phenomena on Tore Supra ICRF antennas investigated by optical diagnostics , 2003 .

[20]  T. Fujita,et al.  Key quantities for ITB formation and sustainment , 2003 .

[21]  J.-W. Ahn,et al.  Integrated Modelling for Steady State Spherical Tokamaks , 2003 .

[22]  A. Field,et al.  Confinement and exhaust in the Mega Ampere Spherical Tokamak , 2002 .

[23]  T. Fülöp,et al.  Effect of poloidal density variation of neutral atoms on the tokamak edge. , 2002, Physical review letters.

[24]  F. Jenko,et al.  Prediction of significant tokamak turbulence at electron gyroradius scales. , 2002, Physical review letters.

[25]  G. F. Counsell,et al.  H-mode access and performance in the Mega-Amp Spherical Tokamak , 2002 .

[26]  K. McClements,et al.  Excitation of axisymmetric Alfvénic modes in Ohmic tokamak discharges , 2002 .

[27]  J. Ahn,et al.  Boundary plasma and divertor phenomena in MAST , 2002 .

[28]  X. Litaudon,et al.  A dimensionless criterion for characterizing internal transport barriers in JET , 2002 .

[29]  F. Ryter,et al.  Progress of the international H-mode power threshold database activity , 2002 .

[30]  G. F. Counsell,et al.  H-mode plasmas in the MAST spherical tokamak , 2002 .

[31]  M. Valovič,et al.  Inboard gas puffing and behaviour of H-mode edge parameters in COMPASS-D , 2002 .

[32]  M. Cox,et al.  Neutral beam heating in the START spherical tokamak , 2002 .

[33]  C. Roach,et al.  L-H transition in the mega-amp spherical tokamak. , 2002, Physical review letters.

[34]  J. Connor,et al.  On the density limit in tokamaks , 2002 .

[35]  Xavier Bonnin,et al.  Modelling of electric fields in tokamak edge plasma and L-H transition , 2002 .

[36]  E. D. Fredrickson,et al.  Initial studies of core and edge transport of NSTX plasmas , 2001 .

[37]  R. White,et al.  Ion heating by fast-particle-induced Alfvén turbulence. , 2001, Physical review letters.

[38]  S. Voskoboynikov,et al.  Simulation of tokamak edge plasma including self-consistent electric fields , 2001 .

[39]  C. Roach,et al.  Confinement in START beam heated discharges , 2001 .

[40]  T. J. Martin,et al.  Steady state operation of spherical tokamaks , 2000 .

[41]  P. Stangeby,et al.  The Plasma Boundary of Magnetic Fusion Devices , 2000 .

[42]  C. Roach,et al.  Magneto-hydro-dynamic limits in spherical tokamaks , 1999 .

[43]  G. Fishpool Loss of confinement due to reduction of the edge pedestal in JET , 1998 .

[44]  A. Loarte,et al.  The impact of ELMs on the ITER divertor , 1998 .

[45]  R. L. Miller,et al.  Magnetohydrodynamic stability of tokamak edge plasmas , 1998 .

[46]  M. Gryaznevich,et al.  Achievement of Record β in the START Spherical Tokamak , 1998 .

[47]  C. Roach,et al.  High-performance discharges in the Small Tight Aspect Ratio Tokamak (START) , 1998 .

[48]  W. Houlberg,et al.  Bootstrap current and neoclassical transport in tokamaks of arbitrary collisionality and aspect ratio , 1997 .

[49]  A. Sykes High β produced by neutral beam injection in the START (Small Tight Aspect Ratio Tokamak) spherical tokamak , 1997 .

[50]  Y. Kamada,et al.  Effect of edge neutrals on the condition of the H-mode transition in JT-60U , 1996 .

[51]  J. F. Briesmeister MCNP-A General Monte Carlo N-Particle Transport Code , 1993 .

[52]  P. C. Stangeby,et al.  Monte Carlo modelling of impurity ion transport for a limiter source/sink , 1988 .

[53]  F. Hinton,et al.  Neoclassical ion transport in rotating axisymmetric plasmas , 1985 .

[54]  R. J. Hawryluk,et al.  An Empirical Approach to Tokamak Transport , 1981 .

[55]  F. Hinton,et al.  Theory of plasma transport in toroidal confinement systems , 1976 .