The Moment Approach to Solve the Drift-Kinetic Equation for Impurity Ions in the Plasma Edge Region

1992 ◽  
Vol 32 (3-4) ◽  
pp. 290-296 ◽  
Author(s):  
H. A. Claaßen ◽  
H. Gerhauser
2004 ◽  
Vol 20 (4) ◽  
pp. 439-456 ◽  
Author(s):  
Jean-Bernard Lasserre ◽  
Tomás Prieto-Rumeau

2009 ◽  
Vol 55 (2T) ◽  
pp. 185-190
Author(s):  
Y. Higashizono ◽  
Y. Nakashima ◽  
M. Shoji ◽  
N. Nishino ◽  
S. Kobayashi ◽  
...  

2002 ◽  
Vol 42 (6-7) ◽  
pp. 616-621 ◽  
Author(s):  
M. Goto ◽  
S. Morita ◽  
LHD experiment group

2004 ◽  
Vol 14 (10) ◽  
pp. 1561-1583 ◽  
Author(s):  
KARL P. HADELER ◽  
THOMAS HILLEN ◽  
FRITHJOF LUTSCHER

In the Langevin or Ornstein–Uhlenbeck approach to diffusion, stochastic increments are applied to the velocity rather than to the space variable. The density of this process satisfies a linear partial differential equation of the general form of a transport equation which is hyperbolic with respect to the space variable but parabolic with respect to the velocity variable, the Klein–Kramers or simply Kramers equation. This modeling approach allows for a more detailed description of individual movement and orientation dependent interaction than the frequently used reaction diffusion framework.For the Kramers equation, moments are computed, the infinite system of moment equations is closed at several levels, and telegraph and diffusion equations are derived as approximations. Then nonlinearities are introduced such that the semi-linear reaction Kramers equation describes particles which move and interact on the same time-scale. Also for these nonlinear problems a moment approach is feasible and yields nonlinear damped wave equations as limiting cases.We apply the moment method to the Kramers equation for chemotactic movement and obtain the classical Patlak–Keller–Segel model. We discuss similarities between chemotactic movement of bacteria and gravitational movement of physical particles.


1996 ◽  
Vol 36 (4) ◽  
pp. 435-442 ◽  
Author(s):  
V Antoni ◽  
E Martines ◽  
M Bagatin ◽  
D Desideri ◽  
G Serianni

2020 ◽  
Vol 86 (3) ◽  
Author(s):  
Mike F. Martin ◽  
Matt Landreman

Impurity temperature screening is a favourable neoclassical phenomenon involving an outward radial flux of impurity ions from the core of fusion devices. Quasisymmetric magnetic fields lead to intrinsically ambipolar neoclassical fluxes that give rise to temperature screening for low enough $\unicode[STIX]{x1D702}^{-1}\equiv d\ln n/d\ln T$ . In contrast, neoclassical fluxes in generic stellarators will depend on the radial electric field, which is predicted to be inward for ion-root plasmas, potentially leading to impurity accumulation. Here, we examine the impurity particle flux in a number of approximately quasisymmetric stellarator configurations and parameter regimes while varying the amount of symmetry breaking in the magnetic field. For the majority of this work, neoclassical fluxes have been obtained using the SFINCS drift-kinetic equation solver with electrostatic potential $\unicode[STIX]{x1D6F7}=\unicode[STIX]{x1D6F7}(r)$ , where $r$ is a flux-surface label. Results indicate that achieving temperature screening is possible, but unlikely, at low-collisionality reactor-relevant conditions in the core. Thus, the small departures from symmetry in nominally quasisymmetric stellarators are large enough to significantly alter the neoclassical impurity transport. A further look at the magnitude of these fluxes when compared to a gyro-Bohm turbulence estimate suggests that neoclassical fluxes are small in configurations optimized for quasisymmetry when compared to turbulent fluxes.


2014 ◽  
Vol 66 (5) ◽  
Author(s):  
Kei Yamada ◽  
Masaki S. Yamaguchi ◽  
Hideki Asada ◽  
Naoteru Gouda

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