Distribution function of plasma particles in axial magnetic and radial electric fieldsfor the transverse injection of neutral gas
The distribution function of particles in plasma which is created in crossed axial magnetic and radial electric fields by ionization of gas is obtained. It is assumed that the neutral gas before its ionization rotates with a constant angular velocity and the gas particle velocity distribution func...
Збережено в:
| Дата: | 2016 |
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| Автор: | |
| Формат: | Стаття |
| Мова: | English |
| Опубліковано: |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
2016
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| Назва видання: | Вопросы атомной науки и техники |
| Теми: | |
| Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/115328 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | Distribution function of plasma particles in axial magnetic and radial electric fieldsfor the transverse injection of neutral gas / D.V. Chibisov // Вопросы атомной науки и техники. — 2016. — № 6. — С. 104-107. — Бібліогр.: 8 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| Резюме: | The distribution function of particles in plasma which is created in crossed axial magnetic and radial electric
fields by ionization of gas is obtained. It is assumed that the neutral gas before its ionization rotates with a constant
angular velocity and the gas particle velocity distribution function in rotating frame is Maxwellian. Produced plasma
particles move in crossed fields without collisions. The obtained distribution function is written in the coordinates of
the guiding center. The expressions for the distribution function in the various special cases are also obtained. |
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