Titlebook: Cross-Magnetic Turbulent Diffusion of Charged Particles in a Weakly Ionized Plasma; Michio Matsumoto Book 1972 Westdeutscher Verlag GmbH,

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Discussion,ons when the values . are not so small as shown in eq. (23). We will here discuss the values of A for the intermediate region between the small and large amplitude fluctuations by comparing with the succesive method of Kadomtsev.

hypertension

Achtergrondinformatie en basisprincipesre determined by fourth order moments, the fourth order moments by next higher order ones, and so on. For a calculation, we must truncate this hierarchy. Then, we apply a method similar to Millionshchikov’s to the fourth order moments, mentioned before. The validity of this method will be discussed later.

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Interim

R. Boniver,D. C. Alpini,G. Brugnoniter than the plasma frequencies π., where the subscript a stands for the type of the charged particles. Frequencies of the fluctuations are much less than V.. Hence, we assume that the charged particles have almost nearly a local Maxwellian velocity distribution. The charged particles are further affected by electric field fluctuations.

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Basic Consideration,ter than the plasma frequencies π., where the subscript a stands for the type of the charged particles. Frequencies of the fluctuations are much less than V.. Hence, we assume that the charged particles have almost nearly a local Maxwellian velocity distribution. The charged particles are further affected by electric field fluctuations.

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Evalueren met beeldende middelenIf the microscopic state of the plasma at time t is completely determined by the well-known coordinates and velocities of particles, we can start from the Klimontovich equations for the phase densities Na (., ., t).