Titlebook: An Introduction to the Linear Theories and Methods of Electrostatic Waves in Plasmas; W. D. Jones,H. J. Doucet,J. M. Buzzi Book 1985 Sprin

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Landau Damping an Initial-Value Problem, considered as two or more interpenetrating fluids (one for the electrons and one for each ion species). The main disadvantage of this model, as has been pointed out several times, is that only the velocity . of each plasma specie can be taken into account, so that any velocity-dependent effects, su

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Kinetic Theory of Forced Oscillations in a One-Dimensional Warm Plasma,ds to wave excitation by a transparent grid immersed in a uniform plasma and biased at the plasma potential. As in Chapter 7, we will again use the concepts of free-streaming and collective perturbations in the plasma. We will show that, as first pointed out by Hirschfield and Jacobs (1968), the col

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Ion-Acoustic Waves in Maxwellian Plasmas A Boundary-Value Problem,damping was introduced by L. D. Landau (1946) who demonstrated theoretically that if the speed of an acoustic wave in a plasma is slightly larger than the average thermal speed of one of the charge species (either ions or electrons) in the plasma, a wave-particle interaction should occur which would

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Numerical Methods,a conceptual point of view. In this chapter we present some numerical methods that the reader may use on a microcomputer with two benefits: (1) By looking at the numerical solution of a particular problem, the reader may reach a better understanding of some of the theoretical subtleties discussed in

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powerful theoretical and experimental techniques and including a wide range of appli­ cations. As such, it is now frequently introduced in university physics and engineering curricula at the senior and first-year-graduate levels. A necessary prerequisite for all of modern plasma studies is the under­ standin978-1-4757-0213-2978-1-4757-0211-8

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The Cookbook Everything You Always Wanted to Know About Fourier, Laplace, and Hilbert Transforms, brier-Laplace transforms to other equations that must be satisfied by the wave-plasma system allows other quantities, such as ..(.) and ..(.), the first-order perturbations of the particle distribution and particle density, respectively, to be similarly computed in (.) space.

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