Variational approach to radiofrequency waves in magnetic fusion devices

Magnetic fusion plasmas feature two major classes of low frequency electromagnetic oscillations: waves in the ion cyclotron range of frequencies (ICRFs) constitute a well established method employed for plasma heating and current drive, whereas waves in the Alfven range of frequencies naturally occur in the form of modes in close interaction with fast particles. The propagation of these waves is characterized by significant space-dispersion, making it necessary to incorporate non-local effects in the global kinetic full-wave codes which are often employed for their simulation. We present here a variational approach to this problem, which has the advantage of providing a common framework to the wave calculation and to the quasilinear response description. Two important points are discussed: firstly, we show that the irreversible part of the power transferred from the wave to the plasma particles is directly available and does not require an explicit evaluation of the kinetic flux; secondly, it is demonstrated that the symmetry of the obtained plasma functional ensures that these energy transfers are described in a consistent fashion, regardless of the level of approximation employed to evaluate the particle Hamiltonian. Finally, quasi-local, finite Larmor radius expressions are derived in the framework of this formalism and implemented in a new multi-dimensional full-wave code, named EVE, which is employed to analyse two ICRF heating scenarios for ITER.

[1]  Allan N. Kaufman,et al.  Quasilinear Diffusion of an Axisymmetric Toroidal Plasma , 1972 .

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

[3]  A. Samain,et al.  Variational theory of ion cyclotron resonance heating in tokamak plasmas , 1985 .

[4]  D. Swanson Radio frequency heating in the ion‐cyclotron range of frequencies , 1985 .

[5]  Scharer,et al.  Local power conservation for linear wave propagation in an inhomogeneous plasma. , 1985, Physical review letters.

[6]  Kashuba,et al.  Effect of parallel magnetic field gradients on absorption and mode conversion in the ion-cyclotron range of frequencies. , 1988, Physical review letters.

[7]  On the local power dissipation of h.f. waves in hot inhomogeneous plasmas , 1988 .

[8]  Local full-wave energy and quasilinear analysis in nonuniform plasmas , 1989 .

[9]  K. Appert,et al.  Theory of plasma heating by low frequency waves: Magnetic pumping and Alfvén resonance heating , 1991 .

[10]  A. Samain,et al.  Hamiltonian theory of the ion cyclotron minority heating dynamics in tokamak plasmas , 1991 .

[11]  W. Kerner,et al.  Free boundary resistive modes in tokamaks , 1993 .

[12]  Per Helander,et al.  Monte Carlo operators for orbit‐averaged Fokker–Planck equations , 1994 .

[13]  Laurent Villard,et al.  Global waves in resistive and hot tokamak plasmas , 1995 .

[14]  P. U. Lamalle,et al.  On the radiofrequency response of tokamak plasmas , 1997 .

[15]  F. G. Rimini,et al.  D-T fusion with ion cyclotron resonance heating in the JET tokamak , 1998 .

[16]  Marco Brambilla,et al.  Numerical simulation of ion cyclotron waves in tokamak plasmas , 1999 .

[17]  K. Wong,et al.  A review of Alfvén eigenmode observations in toroidal plasmas , 1999 .

[18]  W. Kerner,et al.  CASTOR-K , 1999 .

[19]  ITER relevant ICRF heating scenarios with large ion heating fraction , 2000 .

[20]  Eduardo F. D'Azevedo,et al.  All-orders spectral calculation of radio-frequency heating in two-dimensional toroidal plasmas , 2001 .

[21]  G. T. Hoang,et al.  On the role of ion heating in ICRF heated discharges in Tore Supra , 2001 .

[22]  D. Van Eester,et al.  Re-evaluation of ITER ion cyclotron operating scenarios , 2002 .

[23]  Modelling of Alfvén waves in JET plasmas with the CASTOR-K code* , 2002 .

[24]  Erwin Frederick Jaeger,et al.  Nonlinear fluxes and forces from radio-frequency waves with application to driven flows in tokamaks , 2004 .

[25]  Laurent Villard,et al.  Three-Dimensional Full-Wave Propagation Code for Cold Plasma , 2004 .

[26]  M. J. Mantsinen,et al.  Effects of finite drift orbit width and RF-induced spatial transport on plasma heated by ICRH , 2004 .

[27]  E. Joffrin,et al.  Localized bulk electron heating with ICRF mode conversion in the JET tokamak , 2004 .

[28]  David Smithe,et al.  Self-consistent full-wave and Fokker-Planck calculations for ion cyclotron heating in non-Maxwellian plasmas , 2005 .

[29]  D. N. Smithe,et al.  Effects of non-Maxwellian species on ion cyclotron waves propagation and absorption in magnetically confined plasmas , 2005 .

[30]  S. Pinches,et al.  Kinetic properties of shear Alfven eigenmodes in tokamak plasmas , 2005 .

[31]  F. Meo,et al.  On the parasitic absorption in FWCD experiments in JET ITB plasmas , 2005 .

[32]  Torbjörn Hellsten,et al.  Analysis of a quasilinear model for ion cyclotron interactions in tokamaks , 2006 .

[33]  O. Sauter,et al.  On ion cyclotron current drive for sawtooth control , 2006 .

[34]  A. Polevoi,et al.  Chapter 1: Overview and summary , 2007 .

[35]  Full‐wave modeling of ICRF waves: global and quasi‐local descriptions , 2007 .

[36]  E. D'Azevedo,et al.  Simulation of high-power electromagnetic wave heating in the ITER burning plasma , 2008 .