Properties of charged particle motion equations in crossed fields and Larmor’s theorem
Motion equations of charged particle placed in crossed fields observed in the laboratory frame of reference and in rotating one are compared. It is shown that the motion equation in fields (E, H) in a plane transverse to the magnetic field in a rotating frame has the same form as the motion equatio...
Збережено в:
| Дата: | 2018 |
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| Автор: | |
| 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/123456789/148849 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | Properties of charged particle motion equations in crossed fields and Larmor’s theorem / Yu.N. Yeliseyev // Вопросы атомной науки и техники. — 2018. — № 6. — С. 90-93. — Бібліогр.: 6 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| Резюме: | Motion equations of charged particle placed in crossed fields observed in the laboratory frame of reference and
in rotating one are compared. It is shown that the motion equation in fields (E, H) in a plane transverse to the magnetic field in a rotating frame has the same form as the motion equation in fields of another sstrength (E', H') in the
laboratory frame. The invariant of motion equation under rotation transformation is found. A problem that is more
general than the Larmor’s one is formulated and studied. There are found out the rotation frequency and the condition under which the particle motion equation in the fields (E₁, H₁) in the laboratory frame coincides with the motion
equation in the fields (E₂, H₂) in the rotating frame. |
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