1982Zeitschrift für Naturforschung AOpen access

Numerical Evaluation of Neoclassical Transport in Stellarators at Arbitrary Collisionality

H. Wobig

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Abstract

The neoclassical diffusion losses of an l = 2 stellarator and an advanced stellarator are analysed with a modified version of the Boozer-Kuo-Petravic Monte-Carlo Code. Particle loss and confinement of a monoenergetic ion distribution are determined at arbitrary collisionality under stationary conditions. Special attention is given to the long mean free path regime. Due to the drift motion of localized particles a depopulation of the distribution function around v∥ = 0 occurs. The confinement time is determined by pitch angle scattering in this case. It is analysed under which conditions the 1/v-scaling of diffusion losses arises. A comparison is made between the loss rate of an advanced stellarator and a classical l = 2-stellarator. Also a tokamak with ripple losses is considered

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The neoclassical diffusion losses of an l = 2 stellarator and an advanced stellarator are analysed with a modified version of the Boozer-Kuo-Petravic Monte-Carlo Code. Particle loss and confinement of a monoenergetic ion distribution are determined at arbitrary collisionality under stationary conditions. Special attention is given to the long mean free path regime. Due to the drift motion of localized particles a depopulation of the distribution function around v∥ = 0 occurs. The confinement time is determined by pitch angle scattering in this case. It is analysed under which conditions the 1/v-scaling of diffusion losses arises. A comparison is made between the loss rate of an advanced stellarator and a classical l = 2-stellarator. Also a tokamak with ripple losses is considered

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Available abstract

The neoclassical diffusion losses of an l = 2 stellarator and an advanced stellarator are analysed with a modified version of the Boozer-Kuo-Petravic Monte-Carlo Code. Particle loss and confinement of a monoenergetic ion distribution are determined at arbitrary collisionality under stationary conditions. Special attention is given to the long mean free path regime. Due to the drift motion of localized particles a depopulation of the distribution function around v∥ = 0 occurs. The confinement time is determined by pitch angle scattering in this case. It is analysed under which conditions the 1/v-scaling of diffusion losses arises. A comparison is made between the loss rate of an advanced stellarator and a classical l = 2-stellarator. Also a tokamak with ripple losses is considered

Key concepts: Stellarator, Collisionality, Physics, Diffusion, Ripple, Computational physics, Monte Carlo method, Distribution function

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