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Neoclassical transport in quasi-axially symmetric stellarators
The author presents a numerical and analytic assessment of the transport in two quasi-axially symmetric stellarators, including one variant of the MHH2 class of such devices, and a configuration they refer to as NHH2, closely related to MHH2. Monte Carlo simulation results are compared with expectations from established stellarator neoclassical theory, and with some empirical stellarator scalings, used as an estimate of the turbulent transport which might be expected. From the standpoint of transport, these may be viewed as either tokamaks with large ({delta} {approximately} 1%) but low-n ripple, or as stellarators with small ripple. For NHH2, numerical results are reasonably well explained by analytic neoclassical theory. MHH2 adheres less to assumptions made in most analytic theory, and its numerical results agree less well with theory than those for NHH2. However, for both, the non-axisymmetric contribution to the heat flux is comparable with the symmetric neoclassical contribution, and also falls into the range of the expected anomalous (turbulent) contribution. Thus, it appears effort to further optimize the thermal transport beyond the particular incarnations studied here would be of at most modest utility. However, the favorable thermal confinement relies heavily on the radial electric field. Thus, the present configurations will have a loss cone for trapped energetic ions, so that further optimization may be indicated for large devices of this type
Fast ion transport in quasisymmetric equilibria in the presence of a resonant Alfv\'{e}nic perturbation
Significant progress has been made in designing magnetic fields that provide
excellent confinement of the guiding enter trajectories of alpha particles
using quasisymmetry (QS). Given the reduction in this transport channel, we
assess the impact of resonant Alfv\'{e}n eigenmodes (AEs) on the guiding center
motion. The AE amplitudes are chosen to be consistent with experimental
measurements and large-scale simulations. We evaluate the drift resonance
condition, phase-space island width, and island overlap criterion for
quasisymmetric configurations. Kinetic Poincar\'{e} plots elucidate features of
the transport, including stiff transport above a critical perturbation
amplitude. Our analysis highlights key departures from the AE-driven transport
in tokamaks, such as the avoidance of phase-space island overlap in
quasihelical configurations and the enhanced transport due to wide phase-space
islands in low magnetic shear configurations. In configurations that are closer
to QS, with QS deviations , the transport is
primarily driven by the AE, while configurations that are further from QS,
, experience significant transport due to the
QS-breaking fields in addition to the AE
Effect of magnetic islands on the impurity flows in NCSX geometry
A new physics idea to protect a plasma from impurity ions with the use of magnetic islands can be examined on the new National Compact Stellarator Experiment device (NCSX), which is under construction at Princeton Plasma Physics Laboratory, USA. On the basis of the MHD approach the impurity ions flows are studied in the configuration with the parameters of NCSX with the magnetic islands m / n=5/3 and m / n=6/3 , which can be excited with the trim coils in NCSX. It is shown that solving the flow trajectory equations dr Γ uΞ± =0 can lead us to the conclusion that ion flow trajectories are concentrated in the region of the magnetic islands.ΠΠΎΠ²Ρ ΡΡΠ·ΠΈΡΠ½Ρ ΡΠ΄Π΅Ρ Π·Π°Ρ
ΠΈΡΡΡ ΠΏΠ»Π°Π·ΠΌΠΈ Π²ΡΠ΄ ΠΏΡΠΎΠ½ΠΈΠΊΠ½Π΅Π½Π½Ρ ΡΠΎΠ½ΡΠ² Π΄ΠΎΠΌΡΡΠΊΠΈ Π·Π° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ ΠΌΠ°Π³Π½ΡΡΠ½ΠΈΡ
ΠΎΡΡΡΠΎΠ²ΡΠ² ΠΌΠΎΠΆΠ½Π° ΠΏΠ΅ΡΠ΅Π²ΡΡΠΈΡΠΈ Π² Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Ρ
Π½Π° Π½ΠΎΠ²ΠΎΠΌΡ ΠΏΡΠΈΡΡΡΠΎΡ National Compact Stellarator Experiment (NCSX), ΡΠΊΠΈΠΉ ΡΠΏΠΎΡΡΠ΄ΠΆΡΡΡΡΡΡ Π² Princeton Plasma Physics Laboratory, USA. ΠΠ° ΠΎΡΠ½ΠΎΠ²Ρ ΠΠΠ Π½Π°Π±Π»ΠΈΠΆΠ΅Π½Π½Ρ ΠΏΠΎΡΠΎΠΊΠΈ ΡΠΎΠ½ΡΠ² Π΄ΠΎΠΌΡΡΠΊΠΈ Π²ΠΈΠ²ΡΠ°ΡΡΡΡΡ Π΄Π»Ρ ΠΊΠΎΠ½ΡΡΠ³ΡΡΠ°ΡΡΡ Π· ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ NCSX Π· ΠΌΠ°Π³Π½ΡΡΠ½ΠΈΠΌΠΈ ΠΎΡΡΡΠΎΠ²Π°ΠΌΠΈ Π· Β«Ρ
Π²ΠΈΠ»ΡΠΎΠ²ΠΈΠΌΠΈΒ» ΡΠΈΡΠ»Π°ΠΌΠΈ m / n=5/3 and m / n=6/3, ΡΠΊΡ ΠΌΠΎΠΆΠ½Π° Π·Π±ΡΠ΄ΠΈΡΠΈ ΡΠΏΠ΅ΡΡΠ°Π»ΡΠ½ΠΈΠΌΠΈ ΡΠΎΠΊΠΎΠ²ΡΠΌΠΈ ΠΊΠ°ΡΡΡΠΊΠ°ΠΌΠΈ (trim coils) Ρ NCSX. Π ΡΡΠ΅Π½Π½Ρ ΡΡΠ²Π½ΡΠ½Ρ ΡΡΠ°ΡΠΊΡΠΎΡΡΠΉ ΠΏΠΎΡΠΎΠΊΡΠ² dr Γ uΞ± =0 Π΄ΠΎΠ²ΠΎΠ΄ΠΈΡΡ, ΡΠΎ ΠΏΠΎΡΠΎΠΊΠΈ ΡΠΎΠ½ΡΠ² ΠΌΠΎΠΆΡΡΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΡΠ²Π°ΡΠΈΡΡ Π² ΠΌΠ΅ΠΆΠ°Ρ
ΠΌΠ°Π³Π½ΡΡΠ½ΠΈΡ
ΠΎΡΡΡΠΎΠ²ΡΠ².ΠΠΎΠ²Π°Ρ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΈΠ΄Π΅Ρ - Π·Π°ΡΠΈΡΠΈΡΡ ΠΏΠ»Π°Π·ΠΌΡ ΠΎΡ ΠΏΡΠΎΠ½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΠΏΡΠΈΠΌΠ΅ΡΠ½ΡΡ
ΠΈΠΎΠ½ΠΎΠ² c ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΎΡΡΡΠΎΠ²ΠΎΠ² - ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΏΡΠΎΠ²Π΅ΡΠ΅Π½Π° Π² ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Ρ
Π½Π° Π½ΠΎΠ²ΠΎΠΉ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠ΅ National Compact Stellarator Experiment (NCSX), ΡΡΡΠΎΡΡΠ΅ΠΉΡΡ Π² Princeton Plasma Physics Laboratory, USA. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΠΠ ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΡ ΠΏΠΎΡΠΎΠΊΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΏΡΠΈΠΌΠ΅ΡΠΈ ΠΈΠ·ΡΡΠ°ΡΡΡΡ Π΄Π»Ρ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΈ Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ NCSX Ρ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌΠΈ ΠΎΡΡΡΠΎΠ²Π°ΠΌΠΈ Ρ Β«Π²ΠΎΠ»Π½ΠΎΠ²ΡΠΌΠΈΒ» ΡΠΈΡΠ»Π°ΠΌΠΈ m / n=5/3 ΠΈ m / n=6/3, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½Ρ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΡΠΌΠΈ ΡΠΎΠΊΠΎΠ²ΡΠΌΠΈ ΠΊΠ°ΡΡΡΠΊΠ°ΠΌΠΈ (trim coils) Π² NCSX. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΡΡΠ°Π΅ΠΊΡΠΎΡΠΈΠΉ ΠΏΠΎΡΠΎΠΊΠΎΠ² dr Γ uΞ± =0 ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΠΎΡΠΎΠΊΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΌΠΎΠ³ΡΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠΈΡΠΎΠ²Π°ΡΡΡΡ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΎΡΡΡΠΎΠ²ΠΎΠ²
A symplectic, symmetric algorithm for spatial evolution of particles in a time-dependent field
A symplectic, symmetric, second-order scheme is constructed for particle
evolution in a time-dependent field with a fixed spatial step. The scheme is
implemented in one space dimension and tested, showing excellent adequacy to
experiment analysis.Comment: version 2; 16 p
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