238 research outputs found

    Geometry dependence of stellarator turbulence

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    Reducing turbulent transport in toroidal configurations via shaping

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    Fast ion transport in quasisymmetric equilibria in the presence of a resonant Alfv\'{e}nic perturbation

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    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 Ξ΄B/B0≲10βˆ’3\delta B/B_0 \lesssim 10^{-3}, the transport is primarily driven by the AE, while configurations that are further from QS, Ξ΄B/B0∼10βˆ’2\delta B/B_0 \sim 10^{-2}, 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

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    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.Нову Ρ„Ρ–Π·ΠΈΡ‡Π½Ρƒ Ρ–Π΄Π΅ΡŽ захисту ΠΏΠ»Π°Π·ΠΌΠΈ Π²Ρ–Π΄ проникнСння Ρ–ΠΎΠ½Ρ–Π² Π΄ΠΎΠΌΡ–ΡˆΠΊΠΈ Π·Π° допомогою ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΈΡ… островів ΠΌΠΎΠΆΠ½Π° ΠΏΠ΅Ρ€Π΅Π²Ρ–Ρ€ΠΈΡ‚ΠΈ Π² СкспСримСнтах Π½Π° Π½ΠΎΠ²ΠΎΠΌΡƒ пристрої National Compact Stellarator Experiment (NCSX), який ΡΠΏΠΎΡ€ΡƒΠ΄ΠΆΡƒΡ”Ρ‚ΡŒΡΡ Π² Princeton Plasma Physics Laboratory, USA. На основі ΠœΠ“Π” наблиТСння ΠΏΠΎΡ‚ΠΎΠΊΠΈ Ρ–ΠΎΠ½Ρ–Π² Π΄ΠΎΠΌΡ–ΡˆΠΊΠΈ Π²ΠΈΠ²Ρ‡Π°ΡŽΡ‚ΡŒΡΡ для ΠΊΠΎΠ½Ρ„Ρ–Π³ΡƒΡ€Π°Ρ†Ρ–Ρ— Π· ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ NCSX Π· ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΈΠΌΠΈ островами Π· Β«Ρ…Π²ΠΈΠ»ΡŒΠΎΠ²ΠΈΠΌΠΈΒ» числами m / n=5/3 and m / n=6/3, які ΠΌΠΎΠΆΠ½Π° Π·Π±ΡƒΠ΄ΠΈΡ‚ΠΈ ΡΠΏΠ΅Ρ†Ρ–Π°Π»ΡŒΠ½ΠΈΠΌΠΈ Ρ‚ΠΎΠΊΠΎΠ²Ρ‹ΠΌΠΈ ΠΊΠ°Ρ‚ΡƒΡˆΠΊΠ°ΠΌΠΈ (trim coils) Ρƒ NCSX. Π Ρ–ΡˆΠ΅Π½Π½Ρ Ρ€Ρ–Π²Π½ΡΠ½ΡŒ Ρ‚Ρ€Π°Ρ”ΠΊΡ‚ΠΎΡ€Ρ–ΠΉ ΠΏΠΎΡ‚ΠΎΠΊΡ–Π² dr Γ— uΞ± =0 Π΄ΠΎΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ, Ρ‰ΠΎ ΠΏΠΎΡ‚ΠΎΠΊΠΈ Ρ–ΠΎΠ½Ρ–Π² ΠΌΠΎΠΆΡƒΡ‚ΡŒ концСнтруватися Π² ΠΌΠ΅ΠΆΠ°Ρ… ΠΌΠ°Π³Π½Ρ–Ρ‚Π½ΠΈΡ… островів.Новая физичСская идСя - Π·Π°Ρ‰ΠΈΡ‚ΠΈΡ‚ΡŒ ΠΏΠ»Π°Π·ΠΌΡƒ ΠΎΡ‚ проникновСния примСсных ΠΈΠΎΠ½ΠΎΠ² c использованиСм ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Ρ… островов - ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ ΠΏΡ€ΠΎΠ²Π΅Ρ€Π΅Π½Π° Π² экспСримСнтах Π½Π° Π½ΠΎΠ²ΠΎΠΉ установкС National Compact Stellarator Experiment (NCSX), строящСйся Π² Princeton Plasma Physics Laboratory, USA. На основС ΠœΠ“Π” приблиТСния ΠΏΠΎΡ‚ΠΎΠΊΠΈ ΠΈΠΎΠ½ΠΎΠ² примСси ΠΈΠ·ΡƒΡ‡Π°ΡŽΡ‚ΡΡ для ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ с ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ NCSX с ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹ΠΌΠΈ островами с Β«Π²ΠΎΠ»Π½ΠΎΠ²Ρ‹ΠΌΠΈΒ» числами m / n=5/3 ΠΈ m / n=6/3, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΌΠΎΠ³ΡƒΡ‚ Π±Ρ‹Ρ‚ΡŒ Π²ΠΎΠ·Π±ΡƒΠΆΠ΄Π΅Π½Ρ‹ ΡΠΏΠ΅Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Ρ‚ΠΎΠΊΠΎΠ²Ρ‹ΠΌΠΈ ΠΊΠ°Ρ‚ΡƒΡˆΠΊΠ°ΠΌΠΈ (trim coils) Π² NCSX. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ Ρ‚Ρ€Π°Π΅ΠΊΡ‚ΠΎΡ€ΠΈΠΉ ΠΏΠΎΡ‚ΠΎΠΊΠΎΠ² dr Γ— uΞ± =0 ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΠΏΠΎΡ‚ΠΎΠΊΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΌΠΎΠ³ΡƒΡ‚ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒΡΡ Π² области ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Ρ… островов

    A symplectic, symmetric algorithm for spatial evolution of particles in a time-dependent field

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    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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