Titlebook: Reviews of Plasma Physics; Volume 13 Acad B. B. Kadomtsev Book 1987 Consultants Bureau, New York 1987 Plasma.plasma physics

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Classical Longitudinal Plasma Losses from Open Adiabatic Traps, units. From the standpoint of containment of high-temperature plasma these traps have a large number of attractive properties. These include, first, a high permissible value of ? (ratio of the plasma and magnetic-field pressures), greater simplicity and ease of construction compared with closed sys

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Spectral-Line Broadening in a Plasma,f the natural width (as would be the case for one atom in vacuum), but in a much wider frequency interval Δω. The causes of line broadening are, first, that the observed line is emitted not by an individual atom but by an entire ensemble of atoms whose emission frequencies can differ for various rea

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Electron Cyclotron Plasma Heating in Tokamaks,his purpose are assumed to be high-frequency methods based on feeding energy to the plasma in the form of electromagnetic waves. High frequency (HF) heating is possible in various frequency bands, each with its own advantages and shortcomings [1–6].

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Classical Longitudinal Plasma Losses from Open Adiabatic Traps,tem, and stability to rough hydrodynamic disturbances (in “minimum-B” systems). At the same time, open traps have also substantial shortcomings, principal among which is the considerable loss of plasma along the force lines.

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Particle Dynamics in Magnetic Traps,imov’s ambipolar (tandem mirror) trap [7]. It is one of the so-called open systems of plasma confinement, or traps with “magnetic mirrors,” which will be discussed below. We shall refer to them for brevity simply as traps.

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Spectral-Line Broadening in a Plasma,roadening governs both the half-width of the line and its profile, i.e., the intensity distribution in frequency. The intensity I(ω) of a given line can be represented as the product of the total (integrated over the spectrum) intensity I. by a factor J(ω) that determines the line profile, so that

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