2009
DOI: 10.1088/0029-5515/49/9/095026
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Limitations, insights and improvements to gyrokinetics

Abstract: For a tokamak, we consider gyrokinetic quasineutrality limitations when evaluating the axisymmetric radial electric field; provide an insight by considering the gyrokinetic entropy production restriction on an ion temperature pedestal like that of ITER; and an present an improved hybrid gyrokinetic-fluid treatment valid on slowly evolving transport time scales.

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Cited by 6 publications
(5 citation statements)
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“…While this assumption can be adequate for the L-mode regime, a strong radial electric field is present in the steep edge (pedestal) of a tokamak under H-mode conditions. Assuming that the characteristic length scale for variations of the plasma density is of order L n ∼ ρ θ , the poloidal ion gyroradius, it follows that a strong radial electric field of E r ∼ V T B θ /c is required to sustain pedestal equilibrium [14]. Here, B θ is the poloidal component of the magnetic field, c is the speed of light, and a subsonic pedestal is assumed.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…While this assumption can be adequate for the L-mode regime, a strong radial electric field is present in the steep edge (pedestal) of a tokamak under H-mode conditions. Assuming that the characteristic length scale for variations of the plasma density is of order L n ∼ ρ θ , the poloidal ion gyroradius, it follows that a strong radial electric field of E r ∼ V T B θ /c is required to sustain pedestal equilibrium [14]. Here, B θ is the poloidal component of the magnetic field, c is the speed of light, and a subsonic pedestal is assumed.…”
Section: Introductionmentioning
confidence: 99%
“…Here, B θ is the poloidal component of the magnetic field, c is the speed of light, and a subsonic pedestal is assumed. A radial electric field of this magnitude makes the E × B drift comparable to the poloidal projection of a particle's parallel velocity [14]. Therefore, the resonance condition for the interaction between GAMs and passing ions, and thus the GAM decay rate, can be modified in the steep H-mode pedestal as compared to its L-mode counterpart.…”
Section: Introductionmentioning
confidence: 99%
“…Even though transport barrier formation cannot be explained by long wavelength neoclassical (non-zonal) sheared flow within the flux surface, these flows are predicted [6,7] and experimentally found to play an important role in the suppression of turbulence in transport barriers [8][9][10][11]. Even in turbulence dominated plasmas the relation between the parallel ion flow and the global radial electric field is expected to be neoclassical with a negligible turbulent contribution [12,13]. Experimental tests of predictions for bulk ion and impurity flows based on numerical and analytical neoclassical models have been reported in [14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Reasonable agreement is seen. Catto et al propose a fresh idea, namely how to improve the gyrokinetic codes [19]. In contrast to the typical gyrokinetic treatments, canonical angular momentum is taken as the gyrokinetic radial variable rather than the radial guiding centre location.…”
Section: Other Transport Problemsmentioning
confidence: 99%