Fully electromagnetic nonlinear gyrokinetic equations for tokamak edge turbulence

An energy conserving set of the fully electromagnetic nonlinear gyrokinetic Vlasov equation and Maxwell’s equations, which is applicable to both L-mode turbulence with large amplitude and H-mode turbulence in the presence of high E×B shear has been derived. The phase-space action variational Lie perturbation method ensures the preservation of the conservation laws of the underlying Vlasov–Maxwell system. Generalized ordering takes ρi⪡ρθi∼LE∼Lp⪡R [here ρi is the thermal ion Larmor radius and ρθi=B∕(Bθρi)], as typically observed in the tokamak H-mode edge, with LE and Lp being the radial electric field and pressure gradient lengths. k⊥ρi∼1 is assumed for generality, and the relative fluctuation amplitudes eδϕ∕Ti∼δB∕B are kept up to the second order. Extending the electrostatic theory in the presence of high E×B shear [Hahm, Phys. Plasmas 3, 4658 (1996)], contributions of electromagnetic fluctuations to the particle charge density and current are explicitly evaluated via pullback transformation from the gyro...

[1]  Allan N. Kaufman,et al.  The Darwin Model as a Tool for Electromagnetic Plasma Simulation , 1971 .

[2]  W. W. Lee,et al.  Gyrokinetic approach in particle simulation , 1981 .

[3]  T. Evans,et al.  TRANSPORT BY INTERMITTENCY IN THE BOUNDARY OF THE DIII-D TOKAMAK , 2002 .

[4]  H. Shirai,et al.  Measurement of turbulence decorrelation during transport barrier evolution in a high-temperature fusion plasma. , 2005, Physical review letters.

[5]  H. Sugama Gyrokinetic field theory , 2000 .

[6]  Viktor K. Decyk,et al.  Krylov–Boholiubov Methods and Gyrokinetics , 2001 .

[7]  T. Hahm,et al.  Weak turbulence theory of collisionless trapped electron driven drift instability in tokamaks , 1991 .

[8]  M. Viola,et al.  Exploration of spherical torus physics in the NSTX device , 2000 .

[9]  R. Littlejohn Hamiltonian perturbation theory in noncanonical coordinates , 1982 .

[10]  A. Fukuyama,et al.  Refinement of the gyrokinetic equations for edge plasmas with large flow shears , 2008 .

[11]  F. Hinton,et al.  Poloidal rotation in tokamaks with large electric field gradients , 1995 .

[12]  A. A. Galeev,et al.  Basic plasma physics II , 1983 .

[13]  Gregory W. Hammett,et al.  Toroidal gyrofluid equations for simulations of tokamak turbulence , 1996 .

[14]  J. Manickam,et al.  Nonlocal properties of gyrokinetic turbulence and the role of E×B flow shear , 2007 .

[15]  S. Zweben,et al.  Visible imaging of edge fluctuations in the TFTR tokamak , 1989 .

[16]  Ronald H. Cohen,et al.  Low-to-high confinement transition simulations in divertor geometry , 2000 .

[17]  Robert G. Littlejohn,et al.  Hamiltonian formulation of guiding center motion , 1981 .

[18]  Paul W. Terry,et al.  Influence of sheared poloidal rotation on edge turbulence , 1990 .

[19]  Hahm,et al.  Self-consistency constraints on turbulent magnetic transport and relaxation in a collisionless plasma. , 1986, Physical review letters.

[20]  W. W. Lee,et al.  Nonlinear turbulent transport in magnetic fusion plasmas , 2008 .

[21]  T. S. Hahm,et al.  Zonal flows in plasma—a review , 2005 .

[22]  Laurent Villard,et al.  Full radius linear and nonlinear gyrokinetic simulations for tokamaks and stellarators: zonal flows, applied E × B flows, trapped electrons and finite beta , 2004 .

[23]  W. Tang,et al.  Advanced computations in plasma physics , 2002 .

[24]  R. Hatzky,et al.  Global particle-in-cell simulations of Alfvénic modes , 2008 .

[25]  Alain J. Brizard,et al.  Nonlinear gyrokinetic theory for finite‐beta plasmas , 1988 .

[26]  T. Hahm Physics behind transport barrier theory and simulations , 2002 .

[27]  Dawson,et al.  Fluctuations and transport due to ion-temperature-gradient-driven instabilities. , 1990, Physical review letters.

[28]  P. Catto,et al.  Drift kinetic equation exact through second order in gyroradius expansion , 2005 .

[29]  J. Manickam,et al.  Nonlocal neoclassical transport in tokamak and spherical torus experiments , 2006 .

[30]  P. Catto,et al.  Arbitrary poloidal gyroradius effects in tokamak pedestals and transport barriers , 2008 .

[31]  E. Frieman,et al.  Nonlinear gyrokinetic equations for low-frequency electromagnetic waves in general plasma equilibria , 1981 .

[32]  T. Hahm,et al.  Turbulent transport reduction by zonal flows: massively parallel simulations , 1998, Science.

[33]  Nonlocal nonlinear electrostatic gyrofluid equations , 2004, physics/0410276.

[34]  L. L. LoDestro,et al.  Gyroaveraged equations for both the gyrokinetic and drift‐kinetic regimes , 1992 .

[35]  M. Rosenbluth,et al.  Nonlinear saturation of the dissipative trapped-electron instability , 1977 .

[36]  F. Wagner,et al.  Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor Discharges of the ASDEX Tokamak , 1982 .

[37]  L. Giannone,et al.  Measurements and modelling of electrostatic fluctuations in the scrape-off layer of ASDEX , 1995 .

[38]  A. Fukuyama,et al.  Self‐sustained plasma turbulence due to current diffusion , 1995 .

[39]  Robert G. Littlejohn,et al.  Variational principles of guiding centre motion , 1983, Journal of Plasma Physics.

[40]  T. S. Hahm,et al.  Turbulence spreading and transport scaling in global gyrokinetic particle simulations , 2004 .

[41]  M. Greenwald,et al.  Edge turbulence imaging in the Alcator C-Mod tokamak , 2001 .

[42]  Bruce D. Scott,et al.  Computation of electromagnetic turbulence and anomalous transport mechanisms in tokamak plasmas , 2003 .

[43]  William McCay Nevins,et al.  Geometric gyrokinetic theory for edge plasmasa) , 2007 .

[44]  F. Jenko,et al.  Numerical computation of collisionless drift Alfvén turbulence , 1999 .

[45]  William McCay Nevins,et al.  General Gyrokinetic Equations for Edge Plasmas , 2006 .

[46]  B. Scott Three-Dimensional Computation of Drift Alfven Turbulence , 1997 .

[47]  G. Staebler,et al.  Effects of velocity shear and magnetic shear in the formation of core transport barriers in the DIII-D tokamak , 1998 .

[48]  L. Lao,et al.  Role of the radial electric field in the transition from L (low) mode to H (high) mode to VH (very high) mode in the DIII‐D tokamak* , 1994 .

[49]  Burrell,et al.  Role of edge electric field and poloidal rotation in the L-H transition. , 1990, Physical review letters.

[50]  M. Rosenbluth,et al.  A kinetic theory of trapped‐electron‐driven drift wave turbulence in a sheared magnetic field , 1991 .

[51]  Parker,et al.  Gyrokinetic simulation of ion temperature gradient driven turbulence in 3D toroidal geometry. , 1993, Physical review letters.

[52]  Paul,et al.  Long-wavelength density turbulence in the TFTR tokamak. , 1993, Physical review letters.

[53]  Recent results on turbulence and MHD activity achieved by reflectometry. Invited paper , 2006 .

[54]  K. H. Burrell,et al.  Flow shear induced fluctuation suppression in finite aspect ratio shaped tokamak plasma , 1995 .

[55]  T. Hahm Nonlinear gyrokinetic equations for turbulence in core transport barriers , 1996 .

[56]  Williams,et al.  Scalings of Ion-Temperature-Gradient-Driven Anomalous Transport in Tokamaks. , 1996, Physical review letters.

[57]  Turbulent Equipartition Theory of Toroidal Momentum Pinch , 2007 .

[58]  R. Waltz Numerical simulation of electromagnetic turbulence in tokamaks , 1985 .

[59]  X. Xu Neoclassical simulation of tokamak plasmas using the continuum gyrokinetic code TEMPEST. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[60]  Rowan,et al.  Fluctuation-induced energy flux in the tokamak edge. , 1989, Physical review letters.

[61]  J. Candy Beta scaling of transport in microturbulence simulations , 2005 .

[62]  J. Krommes,et al.  Nonlinear gyrokinetic equations , 1983 .

[63]  Transport control by coherent zonal flows in the core/edge transitional regime. , 2000, Physical review letters.

[64]  Bruce D. Scott The character of transport caused by E×B drift turbulence , 2003 .

[65]  Yang Chen,et al.  Gyrokinetic δf particle simulation of trapped electron mode driven turbulence , 2007 .

[66]  Alain J. Brizard,et al.  Variational principle for nonlinear gyrokinetic Vlasov–Maxwell equations , 2000 .

[67]  T. Aniel,et al.  Electron transport in Tore Supra with fast wave electron heating , 1999 .

[68]  T. S. Hahm,et al.  Bounce-averaged kinetic equations and neoclassical polarization density , 1999 .

[69]  H. Sugama,et al.  Nonlinear electromagnetic gyrokinetic equation for plasmas with large mean flows , 1998 .

[70]  Beer,et al.  Turbulent Fluctuations in TFTR Configurations with Reversed Magnetic Shear. , 1996, Physical review letters.

[71]  T. Hahm Rotation shear induced fluctuation decorrelation in a toroidal plasma , 1994 .

[72]  S. Coda,et al.  Beyond paradigm: Turbulence, transport, and the origin of the radial electric field in low to high confinement mode transitions in the DIII-D tokamak , 1995 .

[73]  K. H. Burrell,et al.  Effects of E×B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices , 1997 .

[74]  T. S. Hahm,et al.  Nonlinear gyrokinetic equations for tokamak microturbulence , 1988 .

[75]  Zhihong Lin,et al.  Neoclassical transport in enhanced confinement toroidal plasmas , 1996 .

[76]  Alain J. Brizard,et al.  Nonlinear gyrokinetic Maxwell-Vlasov equations using magnetic co-ordinates , 1989, Journal of Plasma Physics.

[77]  Choong-Seock Chang,et al.  Spontaneous rotation sources in a quiescent tokamak edge plasma , 2008 .

[78]  W. Horton Drift waves and transport , 1999 .

[79]  K. Burrell,et al.  EXPERIMENTAL CHARACTERIZATION OF COHERENT, RADIALLY-SHEARED ZONAL FLOWS IN THE DIII-D TOKAMAK , 2002 .

[80]  Nazikian,et al.  Radial scale length of turbulent fluctuations in the main core of TFTR plasmas. , 1993, Physical review letters.

[81]  Benjamin A. Carreras,et al.  DYNAMICS OF TRANSITION TO ENHANCED CONFINEMENT IN REVERSED MAGNETIC SHEAR DISCHARGES , 1997 .

[82]  H. Berk,et al.  Velocity Space Instabilities in a Toroidal Geometry , 1967 .

[83]  Liang,et al.  Self-Regulating Shear Flow Turbulence: A Paradigm for the L to H Transition. , 1994, Physical review letters.

[84]  R. Hazeltine Self‐consistent radial sheath , 1989 .

[85]  T. Hahm Flow‐shear‐induced Compton scattering of electron drift instability , 1992 .

[86]  W. Tang,et al.  Nonlinear electromagnetic gyrokinetic equations for rotating axisymmetric plasmas , 1994 .

[87]  T. Hahm Trapped particle dynamics in toroidally rotating plasmas , 1992 .

[88]  T. Hahm,et al.  Short wavelength fluctuations and electron heat conductivity in enhanced reversed shear plasmas , 1997 .

[89]  R. Budny,et al.  Local transport barrier formation and relaxation in reverse-shear plasmas on the Tokamak Fusion Test Reactor , 1997 .

[90]  Alain J. Brizard,et al.  Nonlinear gyrokinetic Vlasov equation for toroidally rotating axisymmetric tokamaks , 1995 .

[91]  X. Garbet,et al.  Scaling laws of density fluctuations at high-k on Tore Supra , 2004 .

[92]  Alain J. Brizard,et al.  Foundations of Nonlinear Gyrokinetic Theory , 2007 .

[93]  A. Baños The guiding centre approximation in lowest order , 1967, Journal of Plasma Physics.

[94]  P. Diamond,et al.  A nonlinear bounce kinetic equation for trapped electrons , 1990 .

[95]  P. Diamond,et al.  Nonlinear gyrokinetic theory of toroidal momentum pinch , 2007 .