Magnetic field generation due to resonance absorption

1976 ◽  
Vol 19 (11) ◽  
pp. 1833 ◽  
Author(s):  
Katsunobu Nishihara ◽  
Yukiharu Ohsawa ◽  
Kunioki Mima ◽  
Toshio Tange
Keyword(s):  
Magnetic Field ◽  
Resonance Absorption ◽  
Magnetic Field Generation ◽  
Field Generation

Magnetic field generation by resonance absorption of light

1977 ◽  
Vol 16 (4) ◽  
pp. 1678-1686 ◽  
Author(s):  
B. Bezzerides ◽  
D. F. DuBois ◽  
D. W. Forslund
Keyword(s):  
Magnetic Field ◽  
Resonance Absorption ◽  
Magnetic Field Generation ◽  
Field Generation ◽  
Absorption Of Light

Magnetic Field Generation in Resonance Absorption of Light

1977 ◽  
Vol 38 (9) ◽  
pp. 495-498 ◽  
Author(s):  
B. Bezzerides ◽  
D. F. DuBois ◽  
D. W. Forslund ◽  
E. L. Lindman
Keyword(s):  
Magnetic Field ◽  
Resonance Absorption ◽  
Magnetic Field Generation ◽  
Field Generation ◽  
Absorption Of Light

On Ultrahigh Magnetic-Field Generation Using Solid-State Liner System

2010 ◽  
Vol 38 (8) ◽  
pp. 1719-1722 ◽  
Author(s):  
Victor D Selemir ◽  
Vasily A Demidov ◽  
Pavel B Repin ◽  
Andrey P Orlov ◽  
Nikolay V Egorov
Keyword(s):  
Magnetic Field ◽  
Solid State ◽  
Magnetic Field Generation ◽  
Field Generation ◽  
Liner System ◽  
Ultrahigh Magnetic Field

scholarly journals DEPENDENCE OF THE MAGNETIC FIELD GENERATION MODELS OF IN MODEL OF A αΩ-DYNAMO ON THE INTENSITY OF A POWER TYPE α GENERATOR

2019 ◽  
pp. 58-66
Author(s):  
А.Н. Годомская ◽  
О.В. Шереметьева
Keyword(s):  
Magnetic Field ◽  
Comparative Analysis ◽  
Velocity Field ◽  
Dynamic Model ◽  
Radial Component ◽  
Magnetic Field Generation ◽  
Power Type ◽  
Exponential Kernel ◽  
Field Generation ◽  
The Magnetic Field

В динамической модели -динамо с переменной интенсивностью -генератора моделируются инверсии магнитного поля. Изменение интенсивности -генератора как следствие синхронизации высших мод поля скоростей и магнитного поля регулируется функцией Z(t) со степенным ядром. Получены режимы динамо для двух видов радиальной составляющей в скалярной параметризации -эффекта. Проведён анализ результатов в зависимости от изменения показателя степени ядра функции Z(t), а также сравнительный анализ с результатами исследования 10, где использовано показательное ядро функциии Z(t). In the dynamic model -dimensions are simulated reversions of the magnetic field with a varying intensity of the -generator. The change of the -generator intensity as a result of synchronization of higher modes of the velocity field and the magnetic field is regulated by a function Z(t) with a power kernel. Dynamo modes are obtained for two types of radial component in the scalar parameterization of the -effect. The results were analyzed depending on the change in the exponent of the kernel of the function Z(t), also a comparative analysis with the results of the study 10, where the exponential kernel of the function Z(t) was used.

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