Abstract. The neoclassical return current and parallel viscosity due to the radial electric field (non-equilibrium poloidal rotation) in tokamaks are calculated using the 5-D (3-D in configuration space and 2-D in velocity space) Monte Carlo code ASCOT. Results are compared with the known neoclassical non-ambipolar return current expressions by Shaing [Phys. Fluids B 2 (1990) 2847] and Stringer [Nucl. Fusion 33 (1993) 1249] over a wide range of poloidal Mach numbers Mp = Er/(vtiBθ) and for various collisionalities. Here, vti is the ion thermal velocity, Er is the radial electric field and Bθ is the poloidal magnetic field. Quantitative differences exist due to a simpler collision operator and the various other approximations used in derivin...
A novel method to obtain the full neoclassical transport matrix for general toroidal plasmas by usin...
Calculations of collisional thermal and particle diffusivities in toroidal magnetic plasma confineme...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
The neoclassical return current and parallel viscosity due to the radial electric field (non-equilib...
Non-axisymmetric magnetic perturbations can fundamentally change neoclassical transport in tokamaks ...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
Accurate calculation of perturbed distribution function #14;δf and perturbed magnetic fi eld #14;δB ...
A numerical method is presented for evaluation of the radial diffusion coefficient, based on the ful...
Parallel viscosity ⟨B⋅∇⋅Πi⟩ as a function of radial electric field Er (or, equivalently, nonequilibr...
Knowledge of poloidal velocity is necessary for the determination of the radial electric field, Er, ...
Neoclassical toroidal viscosities (NTVs) in tokamaks are investigated using a δf Monte Carlo simulat...
The neoclassical electric field in a tokamak is determined by the conservation of toroidal angular m...
"A novel method to obtain the full neoclassical transport matrix for general toroidal plasmas by us...
The progress in a 3-dimensional, non-local neoclassical transport simulation code “FORTEC-3D” is des...
In this paper, we present a method for noninductive current drive studies based on three-dimensional...
A novel method to obtain the full neoclassical transport matrix for general toroidal plasmas by usin...
Calculations of collisional thermal and particle diffusivities in toroidal magnetic plasma confineme...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
The neoclassical return current and parallel viscosity due to the radial electric field (non-equilib...
Non-axisymmetric magnetic perturbations can fundamentally change neoclassical transport in tokamaks ...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
Accurate calculation of perturbed distribution function #14;δf and perturbed magnetic fi eld #14;δB ...
A numerical method is presented for evaluation of the radial diffusion coefficient, based on the ful...
Parallel viscosity ⟨B⋅∇⋅Πi⟩ as a function of radial electric field Er (or, equivalently, nonequilibr...
Knowledge of poloidal velocity is necessary for the determination of the radial electric field, Er, ...
Neoclassical toroidal viscosities (NTVs) in tokamaks are investigated using a δf Monte Carlo simulat...
The neoclassical electric field in a tokamak is determined by the conservation of toroidal angular m...
"A novel method to obtain the full neoclassical transport matrix for general toroidal plasmas by us...
The progress in a 3-dimensional, non-local neoclassical transport simulation code “FORTEC-3D” is des...
In this paper, we present a method for noninductive current drive studies based on three-dimensional...
A novel method to obtain the full neoclassical transport matrix for general toroidal plasmas by usin...
Calculations of collisional thermal and particle diffusivities in toroidal magnetic plasma confineme...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...