Discretized collision operator for simulations of fusion non-maxwellian plasma relaxation
The plasma observed in modern fusion devices very often exhibits strongly non-Maxwellian distribution. This is the result of magnetic field lines reconnection with formation of magnetic resonant structures like magnetic islands and stochastic layers. Along with that, the plasma heating by means of...
Збережено в:
Дата: | 2018 |
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Автори: | , , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
2018
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Назва видання: | Вопросы атомной науки и техники |
Теми: | |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/148865 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Discretized collision operator for simulations of fusion non-maxwellian plasma relaxation / O.A. Shyshkin, D.V. Vozniuk, I.O. Girka // Вопросы атомной науки и техники. — 2018. — № 6. — С. 101-104. — Бібліогр.: 10 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | The plasma observed in modern fusion devices very often exhibits strongly non-Maxwellian distribution. This
is the result of magnetic field lines reconnection with formation of magnetic resonant structures like magnetic
islands and stochastic layers. Along with that, the plasma heating by means of neutral beam injection (NBI) and
ion/electron cyclotron resonance frequency (ICRF/ECRF) heating induce the non-Maxwellian fast ions. In order to
get the comprehensive description of plasmas one should take care of plasma particles interaction, i.e. Coulomb
collisions in non-Maxwellian environment. In present paper the expression for the discretized collision operator of a
general Monte Carlo equivalent form in terms of expectation values and standard deviation for the non-Maxwellian
bulk distribution function is derived for a magnetized plasma assuming distribution function isotropy. The
simulation for relaxation of fusion product fractions like -particles, protons and deuterium ions on background
plasma particles is performed with the use of presented collision operator. On this purpose the δ-function
distribution for the bulk plasmas is assumed. |
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